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String Theory
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Andrew Zimmerman Jones
Physics Guide, About.com
with Daniel Robbins, PhD in Physics
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String Theory
FOR
DUMrtlEfif
by Andrew Zimmerman Jones
with Daniel Robbins, PhD in Physics
Wiley Publishing, Inc.
String Theory For Dummies®
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About the Author
Andrew Zimmerman Jones is the Physics Guide at About.com,
a New York Times Company, where he writes and edits news
and articles on all areas of physics. He spends his days working
as an editor for an educational assessment company. He holds a
bachelor's degree in physics from Wabash College, where he also
studied mathematics and philosophy, and a master's degree in
mathematical education from Purdue University.
In addition to work for About.com, Andrew has written a number
of nonfiction essays and reviews, which have appeared in The
Internet Review of Science Fiction, EpicSFF.com, Pink Floyd and
Philosophy, Black Gate, and Heroes and Philosophy. His fiction
credits include short stories in Abyss and Apex, KidVisions, The
Four Bubbas of the Apocalypse, and International House ofBubbas.
He has been a member of Mensa since the eighth grade and has
been intensely interested in both science and science fiction since
even earlier. Along the way, he's also become an Eagle Scout, a
Master Mason in the Freemasons, and won the Harold Q. Fuller
Prize in Physics at Wabash College. His plan for world domination
nears completion with the publication of this book.
Andrew lives in central Indiana with his beautiful wife, Amber,
and son, Elijah. When he's not writing or editing, he is most often
found reading, playing games, watching television, investigating
bizarre scientific phenomena, or updating his personal Web page,
which can be found at www . az j ones . info. Andrew also regularly
reports on any new string theory implications on his Web site at
physics . about . com.
Dedication
This book is dedicated to my loving and lovely wife,
Amber Eckert-Jones. While physicists still search for a law to
unify all of the forces in the physical universe, I don't need to,
because all the forces in my universe come together in you.
Author's Acknowledgments
1 must first profoundly thank my agent, Barb Doyen, for approaching
me with this project. My deepest thanks and appreciations go out
to the wonderful editorial staff at Wiley: Alissa Schwipps for her
valuable input at every step in the process, Vicki Adang for her
ability to turn my scientific babble into coherent explanations, and
Stacy Kennedy for gathering together such a great team in the first
place. I also very much appreciated the constructive and at times
critical input of Dr. Rolf Schimmrigk of Indiana University, South
Bend, who provided initial technical editing on the book. In
addition, I'm profoundly thankful for the extremely detailed
technical expertise, review, and frequent discussions offered by
Dr. Daniel Robbins of the Weinberg Theory Group at the University
of Texas at Austin.
Without the wonderful staff at About.com, notably the Education
Channel editor Madeleine Burry, I would never have had the
opportunity to grow as a writer in this field. Also to author Robert
J. Sawyer, for his mentorship and friendship over the years.
Thanks to you all!
Many thanks to physicists Lee Smolin and John W. Moffat of the
Perimeter Institute for Theoretical Physics, Leonard Susskind of
Stanford University, and Sylvester James Gates, director of the
University of Maryland's Center for String and Particle Theory,
for e-mail exchanges that have helped to clarify various points
throughout the writing of this book.
Finally, my thanks go out to my wife, Amber, and son, Elijah, for
putting up with me, even when I was driven frantic by deadlines.
Thanks also to my mother, Nancy Zimmerman, and mother-in-law,
Tina Lewis, for their help in keeping the family entertained while I
worked feverishly in the basement.
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Contents at a Glance
Introduction 7
Part 1: Introducing String Theory 7
Chapter 1: So What Is String Theory Anyway? 9
Chapter 2: The Physics Road Dead Ends at Quantum Gravity 25
Chapter 3: Accomplishments and Failures of String Theory 39
Part 11: The Physics Upon Which
String Theory Is Built k9
Chapter 4: Putting String Theory in Context: Understanding
the Method of Science 51
Chapter 5: What You Must Know about Classical Physics 63
Chapter 6: Revolutionizing Space and Time: Einstein's Relativity 81
Chapter 7: Brushing Up on Quantum Theory Basics 99
Chapter 8: The Standard Model of Particle Physics 1 19
Chapter 9: Physics in Space: Considering Cosmology and Astrophysics 137
Part 111: Building String Theory:
A Theory of Everything 159
Chapter 10: Early Strings and Superstrings:
Unearthing the Theory's Beginnings 161
Chapter 11: M-Theory and Beyond: Bringing String Theory Together 183
Chapter 12: Putting String Theory to the Test 209
Part IV: The Unseen Cosmos: String Theory On the
Boundaries of Knowledge 227
Chapter 13: Making Space for Extra Dimensions 229
Chapter 14: Our Universe — String Theory, Cosmology, and Astrophysics 245
Chapter 15: Parallel Universes: Maybe You Can Be Two Places at Once 261
Chapter 16: Have Time, Will Travel 275
Part V: What the Other Guys Say:
Criticisms and Alternatives 295
Chapter 17: Taking a Closer Look at the String Theory Controversy 297
Chapter 18: Loop Quantum Gravity: String Theory's Biggest Competitor 313
Chapter 19: Considering Other Ways to
Explain the Universe 323
Part VI: The Part of Tens 337
Chapter 20: Ten Questions a Theory of Everything Should (Ideally) Answer 339
Chapter 21: Ten Notable String Theorists 345
Index 351
Table of Contents
Introduction 7
About This Book 1
Conventions Used in This Book 2
What You're Not to Read 3
Foolish Assumptions 3
How This Book Is Organized 4
Part I: Introducing String Theory 4
Part II: The Physics Upon Which String Theory Is Built 4
Part III: Building String Theory: A Theory of Everything 5
Part IV: The Unseen Cosmos: String Theory
on the Boundaries of Knowledge 5
Part V: What the Other Guys Say: Criticism and Alternatives 5
Part VI: The Part of Tens 5
Icons Used in this Book 6
Where to Go from Here 6
Parti: Introducing String Theory 7
Chapter 1: So What Is String Theory Anyway? 9
String Theory: Seeing What Vibrating Strings Can Tell Us about the
Universe 9
Using tiny and huge concepts to create a theory of everything.... 10
A quick look at where string theory has been 11
Introducing the Key Elements of String Theory 12
Strings and branes 12
Quantum gravity 14
Unification of forces 14
Supersymmetry 15
Extra dimensions 15
Understanding the Aim of String Theory 16
Explaining matter and mass 16
Defining space and time 17
Quantizing gravity 18
Unifying forces 18
String Theory For Dummies _
Appreciating the Theory's Amazing (and Controversial)
Implications 19
Landscape of possible theories 19
Parallel universes 20
Wormholes 20
The universe as a hologram 21
Time travel 21
The big bang 21
The end of the universe 22
Why Is String Theory So Important? 22
Chapter 2: The Physics Road Dead Ends at Quantum Gravity 25
Understanding Two Schools of Thought on Gravity 26
Newton's law of gravity: Gravity as force 26
Einstein's law of gravity: Gravity as geometry 28
Describing Matter: Physical and Energy-Filled 28
Viewing matter classically: Chunks of stuff 29
Viewing matter at a quantum scale: Chunks of energy 29
Grasping for the Fundamental Forces of Physics 30
Electromagnetism: Super-speedy energy waves 30
Nuclear forces: What the strong force joins,
the weak force tears apart 31
Infinities: Why Einstein and the Quanta Don't Get Along 32
Singularities: Bending gravity to the breaking point 33
Quantum jitters: Space-time under a quantum microscope 33
Unifying the Forces 35
Einstein's failed quest to explain everything 35
A particle of gravity: The graviton 36
Supersymmetry's role in quantum gravity 37
Chapter 3: Accomplishments and Failures of String Theory 39
Celebrating String Theory's Successes 39
Predicting gravity out of strings 40
Explaining what happens to a black hole (sort of) 40
Explaining quantum field theory using string theory 41
Like John Travolta, string theory keeps making a comeback 41
Being the most popular theory in town 42
Considering String Theory's Setbacks 43
The universe doesn't have enough particles 43
Dark energy: The discovery string theory
should have predicted 44
Where did all of these "fundamental" theories come from? 45
Looking into String Theory's Future 45
Theoretical complications: Can we figure out string theory? 46
Experimental complications: Can we prove string theory? 46
Table of Contents ^/
Part 11: The Physics Upon Which String Theory Is Built... b9
Chapter 4: Putting String Theory in Context: Understanding
the Method of Science 51
Exploring the Practice of Science 52
The myth of the scientific method 52
The need for experimental falsifiability 53
The foundation of theory is mathematics 55
The rule of simplicity 56
The role of objectivity in science 57
Understanding How Scientific Change Is Viewed 57
Old becomes new again: Science as revolution 58
Combining forces: Science as unification 59
What happens when you break it? Science as symmetry 60
Chapter 5: What You Must Know about Classical Physics 63
This Crazy Little Thing Called Physics 63
No laughing matter: What we're made of 64
Add a little energy: Why stuff happens 66
Symmetry: Why some laws were made to be broken 67
All Shook Up: Waves and Vibrations 68
Catching the wave 69
Getting some good vibrations 70
Newton's Revolution: How Physics Was Born 72
Force, mass, and acceleration: Putting objects into motion 73
Gravity: A great discovery 74
Optics: Shedding light on light's properties 75
Calculus and mathematics: Enhancing scientific understanding .... 75
The Forces of Light: Electricity and Magnetism 75
Light as a wave: The ether theory 76
Invisible lines of force: Electric and magnetic fields 76
Maxwell's equations bring it all together:
Electromagnetic waves 79
Two dark clouds and the birth of modern physics 80
Chapter 6: Revolutionizing Space and Time: Einstein's Relativity . . .81
What Waves Light Waves? Searching for the Ether 82
No Ether? No Problem: Introducing Special Relativity 84
Unifying space and time 85
Unifying mass and energy 87
Changing Course: Introducing General Relativity 89
Gravity as acceleration 89
Gravity as geometry 91
Testing general relativity 92
Applying Einstein's Work to the Mysteries of the Universe 95
Kaluza-Klein Theory — String Theory's Predecessor 96
}ff f String Theory For Dummies _
Chapter 7: Brushing Up on Quantum Theory Basics 99
Unlocking the First Quanta: The Birth of Quantum Physics 100
Fun with Photons: Einstein's Nobel Idea of Light 102
Waves and Particles Living Together 105
Light as a wave: The double slit experiment 105
Particles as a wave: The de Broglie hypothesis 106
Quantum physics to the rescue: The quantum wavefunction 108
Why We Can't Measure It All: The Uncertainty Principle 109
Dead Cats, Live Cats, and Probability in Quantum Physics Ill
Does Anyone Know What Quantum Theory Means? 112
Interactions transform quantum systems:
The Copenhagen interpretation 113
If no one's there to see it, does the universe exist?
The participatory anthropic principle 113
All possibilities take place: The many worlds interpretation 114
What are the odds? Consistent histories 115
Searching for more fundamental data:
The hidden variables interpretation 115
Quantum Units of Nature — Planck Units 116
Chapter 8: The Standard Model of Particle Physics 119
Atoms, Atoms, Everywhere Atoms: Introducing Atomic Theory 120
Popping Open the Atomic Hood and Seeing What's Inside 121
Discovering the electron 122
The nucleus is the thing in the middle 123
Watching the dance inside an atom 123
The Quantum Picture of the Photon: Quantum Electrodynamics 125
Dr. Feynman's doodles explain how particles
exchange information 125
Discovering that other kind of matter: Antimatter 127
Sometimes a particle is only virtual 128
Digging into the Nucleus: Quantum Chromodynamics 129
The pieces that make up the nucleus: Nucleons 129
The pieces that make up the nucleon's pieces: Quarks 130
Looking into the Types of Particles 131
Particles of force: Bosons 131
Particles of matter: Fermions 132
Gauge Bosons: Particles Holding Other Particles Together 133
Exploring the Theory of Where Mass Comes From 134
From Big to Small: The Hierarchy Problem in Physics 135
Chapter 9: Physics in Space: Considering
Cosmology and Astrophysics 137
Creating an Incorrect Model of the Universe 138
Aristotle assigns realms to the universe 138
Ptolemy puts Earth at the center of the
universe (and the Catholic Church agrees) 139
_ Table of Contents tffff
The Enlightened Universe: Some Changes Allowed 141
Copernicus corrects what's where in the universe 141
Beholding the movements of heavenly bodies 142
Introducing the Idea of an Expanding Universe 143
Discovering that energy and pressure have gravity 143
Hubble drives it home 145
Finding a Beginning: The Big Bang Theory 146
Bucking the big bang: The steady state theory 147
Going to bat for the big bang: Cosmic microwave
background radiation 148
Understanding where the chemical elements came from 150
Using Inflation to Solve the Universe's Problems of
Flatness and Horizon 150
The universe's issues: Too far and too flat 151
Rapid expansion early on holds the solutions 152
Dark Matter: The Source of Extra Gravity 153
Dark Energy: Pushing the Universe Apart 153
Stretching the Fabric of Space-Time into a Black Hole 156
What goes on inside a black hole? 156
What goes on at the edge of a black hole? 157
Part 111: Building String Theory:
A Theory of Everything 159
Chapter 10: Early Strings and Superstrings:
Unearthing the Theory's Beginnings 161
Bosonic String Theory: The First String Theory 161
Explaining the scattering of particles with
early dual resonance models 162
Exploring the first physical model: Particles as strings 164
Bosonic string theory loses out to the Standard Model 165
Why Bosonic String Theory Doesn't Describe Our Universe 166
Massless particles 166
Tachyons 167
No electrons allowed 168
25 space dimensions, plus 1 of time 168
Supersymmetry Saves the Day: Superstring Theory 170
Fermions and bosons coexist . . . sort of 171
Double your particle fun: Supersymmetry
hypothesizes superpartners 172
Some problems get fixed, but the dimension problem remains.... 173
Supersymmetry and Quantum Gravity in the Disco Era 174
The graviton is found hiding in string theory 174
The other supersymmetric gravity theory: Supergravity 176
String theorists don't get no respect 176
A Theory of Everything: The First Superstring Revolution 177
}C((/ String Theory For Dummies _
But We've Got Five Theories!
Type I string theory
Type IIA string theory
Type IIB string theory
Two strings in one: Heterotic strings
How to Fold Space: Introducing Calabi-Yau Manifolds
String Theory Loses Steam
Chapter 11: M-Theory and Beyond:
Bringing String Theory Together
Introducing the Unifying Theory: M-Theory
Translating one string theory into another: Duality
Using two dualities to unite five superstring theories
The second superstring revolution begins:
Connecting to the 11-dimensional theory
Branes: Stretching Out a String
The discovery of D-branes: Giving open strings
something to hold on to
Creating particles from p-branes
Deducing that branes are required by M-theory
Uniting D-branes and p-branes into one type of brane
Using branes to explain black holes
Getting stuck on a brane: Brane worlds
Matrix Theory as a Potential M-Theory
Gaining Insight from the Holographic Principle
Capturing multidimensional information on a flat surface....
Connecting the holographic principle to our reality
Considering AdS/CFT correspondence 199
String Theory Gets Surprised by Dark Energy 200
Considering Proposals for Why Dimensions Sometimes Uncurl 201
Measurable dimensions 202
Infinite dimensions: Randall-Sundrum models 202
Understanding the Current Landscape: A Multitude of Theories 204
The anthropic principle requires observers 204
Disagreeing about the principle's value 207
Chapter 12: Putting String Theory to the Test 209
Understanding the Obstacles 210
Testing an incomplete theory with indistinct predictions 210
Test versus proof 211
Testing Supersymmetry 211
Finding the missing sparticles 212
Testing implications of supersymmetry 212
Testing Gravity from Extra Dimensions 213
Testing the inverse square law 214
Searching for gravity waves in the CMBR 214
_ Table of Contents %(/
Disproving String Theory Sounds Easier Than It Is 215
Violating relativity 215
Mathematical inconsistencies 216
Could Proton Decay Spell Disaster? 217
Looking for Evidence in the Cosmic Laboratory:
Exploring the Universe 218
Using outer space rays to amplify small events 218
Analyzing dark matter and dark energy 222
Detecting cosmic superstrings 222
Looking for Evidence Closer to Home: Using Particle Accelerators 223
Relativistic Heavy Ion Collider (RHIC) 224
Large Hadron Collider (LHC) 224
Colliders of the future 226
Part IV: The Unseen Cosmos: String Theory On the
Boundaries of Knowledge 227
Chapter 13: Making Space for Extra Dimensions 229
What Are Dimensions? 229
2-Dimensional Space: Exploring the Geometry of Flatland 230
Euclidean geometry: Think back to high school geometry 231
Cartesian geometry: Merging algebra and Euclidean geometry .... 231
Three Dimensions of Space 233
A straight line in space: Vectors 233
Twisting 2-dimensional space in three dimensions:
The Mobius strip 234
More twists in three dimensions: Non-Euclidean geometry 236
Four Dimensions of Space-Time 237
Adding More Dimensions to Make a Theory Work 238
Sending Space and Time on a Bender 239
Are Extra Dimensions Really Necessary? 240
Offering an alternative to multiple dimensions 241
Weighing fewer dimensions against simpler equations 242
Chapter 14: Our Universe — String Theory, Cosmology, and
Astrophysics 245
The Start of the Universe with String Theory 245
What was before the bang? 246
What banged? 247
Explaining Black Holes with String Theory 250
String theory and the thermodynamics of a black hole 250
String theory and the black hole information paradox 252
The Evolution of the Universe 253
The swelling continues: Eternal inflation 253
The hidden matter and energy 255
}{(/f String Theory For Dummies _
The Undiscovered Country: The Future of the Cosmos 257
A universe of ice: The big freeze 257
From point to point: The big crunch 257
A new beginning: The big bounce 258
Exploring a Finely Tuned Universe 258
Chapter 15: Parallel Universes: Maybe You Can
Be Two Places at Once 261
Exploring the Multiverse: A Theory of Parallel Universes 261
Level 1: If you go far enough, you'll get back home 264
Level 2: If you go far enough, you'll fall into wonderland 265
Level 3: If you stay where you are, you'll run into yourself 267
Level 4: Somewhere over the rainbow, there's a magical land.... 269
Accessing Other Universes 270
A history of hyperspace 270
How quantum mechanics can get us from here to there 272
Chapter 16: Have Time, Will Travel 275
Temporal Mechanics 101: How Time Flies 276
The arrow of time: A one-way ticket 276
Relativity, worldlines, and worldsheets:
Moving through space-time 278
Hawking's chronology protection conjecture:
You're not going anywhere 279
Slowing Time to a Standstill with Relativity 280
Time dilation: Sometimes even the best watches run slow 281
Black hole event horizons: An extra-slow
version of slow motion 282
General Relativity and Wormholes: Doorways in Space and Time 282
Taking a shortcut through space and time with a wormhole 284
Overcoming a wormhole's instability
with negative energy 286
Crossing Cosmic Strings to Allow Time Travel 286
A Two-Timing Science: String Theory Makes
More Time Dimensions Possible 287
Adding a new time dimension 287
Reflecting two-time onto a one-time universe 288
Does two-time physics have any real applications? 289
Sending Messages through Time 290
Time Travel Paradoxes 290
The twin paradox 291
The grandfather paradox 292
Where are the time travelers? 292
_ Table of Contents JC(/H
Part V: What the Other Guus Sau:
Criticisms and Alternatives 295
Chapter 17: Taking a Closer Look at the
String Theory Controversy 297
The String Wars: Outlining the Arguments 298
Thirty years and counting: Framing the debate
from the skeptic's point of view 299
Arise of criticisms 300
Is String Theory Scientific? 301
Argument No. 1: String theory explains nothing 301
Argument No. 2: String theory explains too much 302
Turning a Critical Eye to String Theorists 305
Hundreds of physicists just can't be wrong 305
Holding the keys to the academic kingdom 306
Does String Theory Describe Our Universe? 308
Making sense of extra dimensions 309
Space-time should be fluid 309
How finite is string theory? 310
A String Theory Rebuttal 311
Chapter 18: Loop Quantum Gravity:
String Theory's Biggest Competitor 313
Taking the Loop: Introducing Another Road to Quantum Gravity 313
The great background debate 314
What is looping anyway? 314
Making Predictions with Loop Quantum Gravity 317
Gravity exists (Dun!) 317
Black holes contain only so much space 317
Gamma ray burst radiation travels at different speeds 318
Finding Favor and Flaw with Loop Quantum Gravity 318
The benefit of a finite theorem 318
Spending some time focusing on the flaws 319
So Are These Two Theories the Same with Different Names? 320
Chapter 19: Considering Other Ways to Explain the Universe 323
Taking Other Roads to Quantum Gravity 324
Causal dynamical triangulations (CDT):
If you've got the time, I've got the space 324
Quantum Einstein gravity: Too small to tug 325
Quantum graphity: Disconnecting nodes 326
Internal relativity: Spinning the universe into existence 327
}C(/((( String Theory For Dummies _
Newton and Einstein Don't Make All the Rules:
Modifying the Law of Gravity 328
Doubly special relativity (DSR): Twice
as many limits as ordinary relativity 328
Modified Newtonian dynamics (MOND):
Disregarding dark matter 328
Variable speed of light (VSL): Light used to travel even faster ... 329
Modified gravity (MOG): The bigger the distance,
the greater the gravity 331
Rewriting the Math Books and Physics Books at the Same Time 332
Compute this: Quantum information theory 333
Looking at relationships: Twistor theory 334
Uniting mathematical systems: Noncommutative geometry 334
Part Vh The Part of Tens 337
Chapter 20: Ten Questions a Theory of Everything
Should (Ideally) Answer 339
The Big Bang: What Banged (and Inflated)? 340
Baryon Asymmetry: Why Does Matter Exist? 340
Hierarchy Issues: Why Are There Gaps in Forces,
Particles, and Energy Levels? 341
Fine-Tuning: Why Do Fundamental Constants
Have the Values They Do? 341
Black Hole Information Paradox: What Happens to
Missing Black Hole Matter? 341
Quantum Interpretation: What Does Quantum Mechanics Mean? 342
Dark Mystery No. 1: What Is Dark Matter
(and Why Is There So Much)? 343
Dark Mystery No. 2: What Is Dark Energy (and Why Is It So Weak)? .... 343
Time Symmetry: Why Does Time Seem to Move Forward? 344
The End of the Universe: What Comes Next? 344
Chapter 21: Ten Notable String Theorists 345
Edward Witten 345
John Henry Schwarz 346
Yoichiro Nambu 347
Leonard Susskind 347
David Gross 348
Joe Polchinski 348
Juan Maldacena 348
Lisa Randall 349
MichioKaku 349
Brian Greene 350
Index 351
Introduction
EnJ^y are scientists so excited about string theory? Because string
▼ ▼ theory is the most likely candidate for a successful theory of quantum
gravity — a theory that scientists hope will unite two major physical laws of
the universe into one. Right now, these laws (quantum physics and general
relativity) describe two totally different types of behavior in totally differ-
ent ways, and in the realm where neither theory works completely, we really
don't know what's going on!
Understanding the implications of string theory means understanding pro-
found aspects of our reality at the most fundamental levels. Are there paral-
lel universes? Is there only one law of nature or infinitely many? Why does
our universe follow the laws it does? Is time travel possible? How many
dimensions does our universe possess? Physicists are passionately seeking
answers to these questions.
Indeed, string theory is a fascinating topic, a scientific revolution that prom-
ises to transform our understanding of the universe. As you'll see, these sorts
of revolutions have happened before, and this book helps you understand
how physics has developed in the past, as well as how it may develop in the
future.
This book contains some ideas that will probably, in the coming years, turn
out to be completely false. It contains other ideas that may ultimately prove
to be fundamental laws of our universe, perhaps forming the foundation for
whole new forms of science and technology. No one knows what the future
holds for string theory.
About This Book
In this book, I aim to give a clear understanding of the ever-evolving scien-
tific subfield known as string theory. The media is abuzz with talk about this
"theory of everything," and when you're done with this book you should
know what they're talking about (probably better than they do, most of the
time).
String Theory For Dummies _
In writing this book, I've attempted to serve several masters. First and fore-
most among them has been scientific accuracy, followed closely by entertain-
ment value. Along the way, I've also done my best to use language that you
can understand no matter your scientific background, and I've certainly tried
to keep any mathematics to a minimum.
In writing this book, I set out to achieve the following goals:
(-" Provide the information needed to understand string theory (including
established physics concepts that predate string theory).
v* Establish the successes of string theory so far.
(^ Lay out the avenues of study that are attempting to gain more evidence
for string theory.
J-" Explore the bizarre (and speculative) implications of string theory.
v* Present the critical viewpoints in opposition to string theory, as well as
some alternatives that may bear fruit if it proves to be false.
J-" Have some fun along the way.
j-" Avoid mathematics at all costs. (You're welcome!)
1 hope you, good reader, find that I've been successful at meeting these goals.
And while time may flow in only one direction (Or does it? I explore this in
Chapter 16), your reading of this book may not. String theory is a complex
scientific topic that has a lot of interconnected concepts, so jumping between
concepts is not quite as easy as it may be in some other For Dummies ref-
erence books. I've tried to help you out by including quick reminders and
providing cross-references to other chapters where necessary. So feel free
to wander the pages to your heart's content, knowing that if you get lost you
can work your way back to the information you need.
Contentions Used in This Book
The following conventions are used throughout the text to make things con-
sistent and easy to understand:
Iv* I use monofont for Web sites. Note: When this book was printed, some
Web addresses may have needed to break across two lines of text. If that
happened, rest assured that I haven't put in any extra characters (such
as hyphens) to indicate the break. So, when using one of these Web
addresses, just type in exactly what you see in this book, as though the
line break doesn't exist.
t^ I've done my best not to fill the book with technical jargon, which is
hard to do in a book on one of the most complex and mathematically
driven scientific topics of all time. When I use a technical term, it's in
italics and closely followed by an easy-to-understand definition.
u* Bold is used to highlight key words and phrases in bulleted lists.
Finally, one major convention used in this book is in the title: I use the term
"string theory." In Chapter 10, you discover that string theory is actually
called superstring theory. As you see in Chapter 11, in 1995 physicists real-
ized that the various "string theories" (five existed at the time) included
objects other than strings, called branes. So, strictly speaking, calling it by
the name "string theory" is a bit of a misnomer, but people (including string
theorists themselves) do it all the time, so I'm treading on safe ground. Many
physicists also use the name M-theory to describe string theory after 1995
(although they rarely agree on what the "M" stands for), but, again, I will
mostly refer to it just as "string theory" unless the distinction between differ-
ent types matters.
What llou're Not to Read
All the chapters provide you with important information, but some sections
offer greater detail or tidbits of information that you can skip for now and
come back to later without feeling guilty:
V Sidebars: Sidebars are shaded boxes that give detailed examples or
I explore a tangent in more detail. Ignoring these won't compromise your
understanding of the rest of the material.
\* Anything with a Technical Stuff icon: This icon indicates information
that's interesting but that you can live without. Read these tidbits later if
you're pressed for time.
Foolish Assumptions
About the only assumption that I've made in writing this book is that you're
reading it because you want to know something about string theory. I've tried
to not even assume that you enjoy reading physics books. (I do, but I try not
to project my own strangeness on others.)
I have assumed that you have a passing acquaintance with basic physics
concepts — maybe you took a physics class in high school or have watched
some of the scientific programs about gravity, light waves, black holes, or
other physics-related topics on cable channels or your local PBS station.
You don't need a degree in physics to follow the explanations in this book,
String Theory For Dummies _
although without a degree in physics you might be amazed that anyone can
make sense of any theory this disconnected from our everyday experience.
(Even with physics degree, it can boggle the mind.)
As is customary in string theory books for the general public, the mathemat-
ics has been avoided. You need a graduate degree in mathematics or physics
to follow the mathematical equations at the heart of string theory, and while
I have a graduate degree in mathematics, I've assumed that you don't. Don't
worry — while a complete understanding of string theory is rooted firmly
in the advanced mathematical concepts of quantum field theory, I've used a
combination of text and figures to explain the fascinating ideas behind string
theory.
HovO This Book 1$ Organized
String Theory For Dummies is written so you can easily get to the information
you need, read it, and understand it. It's designed to follow the historical
development of the theory as much as possible, though many of the concepts
in string theory are interconnected. Although I've attempted to make each
chapter understandable on its own, I've included cross-references where con-
cepts repeat to get you back to a more thorough discussion of them.
Part 1: Introducing String Theory
This first part of the book introduces the key concepts of string theory in a
very general way. You read about why scientists are so excited about finding
a theory of quantum gravity. Also, you get your first glimpse into the suc-
cesses and failures of string theory.
Part 11: The Physics Upon Which
String Theory Is Built
String theory is built upon the major scientific developments of the first
70 years or so of the 20th century. In this part, you find out how physicists
(and scientists in general) learn things and what they've learned so far. Part
II includes chapters on how science develops, classical physics (before
Einstein), Einstein's theory of relativity, quantum physics, and the more
recent findings in particle physics and cosmology. The questions raised in
these chapters are those that string theory attempts to answer.
_ Introduction
Part 111: Building String Theory:
A Theory of Everything
You get to the heart of the matter in this part. I discuss the creation and
development of string theory, from 1968 to early 2009. The amazing transfor-
mations of this theory are laid out here. Chapter 12 focuses on ways that the
concepts of string theory can be tested.
Part IV: The Unseen Cosmos: String Theory
on the Boundaries of Knowledge
Here I take string theory out for a spin in the universe, exploring some of the
major concepts in greater detail. Chapter 13 focuses on the concept of extra
dimensions, which are at the core of much of string theory study. Chapter 14
explores the implications for cosmology and how string theory could explain
certain properties of our universe. Even more amazing, in Chapters 15 and
16, you discover what string theory has to say about possible parallel uni-
verses and the potential for time travel.
Part V: What the Other Guys Say:
Criticism and Alternatives
The discussion gets heated in this part as you read about the criticisms of
string theory. String theory is far from proven, and many scientists feel that
it's heading in the wrong direction. Here you find out why and see what alter-
natives they're posing, such as loop quantum gravity (string theory's biggest
competitor). If string theory is wrong, scientists will continue to look for
answers to the questions that it seeks to resolve.
Part VI: The Part of Tens
In the For Dummies tradition, the final chapters of this book present lists of
ten topics. Chapter 20 sums up ten outstanding physics questions that scien-
tists hope any "theory of everything" (including string theory) will answer.
Chapter 21 focuses on ten string theorists who have done a lot to advance
the field, either through their own research or by introducing string theory
concepts to the world through popular books.
String Theory For Dummies _
leans Used in this Book
Throughout the book, you'll find icons in the margins that are designed to
help you navigate the text. Here's what these icons mean:
Although everything in this book is important, some information is more
important than other information. This icon points out information that will
definitely be useful later in the book.
In science, theories are often explained with analogies, thought experiments,
or other helpful examples that present complex mathematical concepts in a
way that is more intuitively understandable. This icon indicates that one of
these examples or hints is being offered.
^jH-STi/j^ Sometimes I go into detail that you don't need to know to follow the basic dis-
&/Y*$\ cussion and is a bit more technical (or mathematical) than you may be inter-
ested in. This icon points out that information, which you can skip without
losing the thread of the discussion.
Where to Go from Here
The For Dummies books are organized in such a way that you can surf
through any of the chapters and find useful information without having to
start at Chapter 1. 1 (naturally) encourage you to read the whole book, but
this structure makes it very easy to start with the topics that interest you
the most.
If you have no idea what string theory is, then I recommend looking at
Chapter 1 as a starting point. If your physics is rusty, pay close attention to
Chapters 5-9, which cover the history and current status of the major phys-
ics concepts that pop up over and over again.
If you're familiar with string theory but want some more details, jump
straight to Chapters 10 and 11, where I explain how string theory came about
and reached its current status. Chapter 12 offers some ways of testing the
theory, while Chapters 13-16 take concepts from string theory and apply
them to some fascinating topics in theoretical physics.
Some of you, however, may want to figure out what all the recent fuss is with
people arguing across the blogosphere about string theory. For that, I recom-
mend jumping straight to Chapter 17, which addresses some of the major
criticisms of string theory. Chapters 18 and 19 focus heavily on other theo-
ries that may either help expand or replace string theory, so they're a good
place to go from there.
Parti
Introducing String
Theory
The 5 th Wave
By Rich Tennant
* Okay— novi that the paramedic is here viith
the defibrillator and smelling salts, prepare
to learn about string theory.*
In this part .
JW/I eet string theory, a bold scientific theory that
/fl attempts to reconcile all the physical properties of
our universe into a single unified and coherent mathemati-
cal framework.
String theory's goal is to make quantum physics and
Einstein's theory of gravity (called general relativity) play
nice. In this part, I explain why scientists want to find a
theory of quantum gravity, and then I review the successes
and failures at applying string theory to this search.
This part is something of an overview for the entire book,
so stick with me. The foundation laid here may help
explain the entire universe.
Chapter 1
So What Is String Theory Anyway?
In This Chapter
Knowing that string theory is based on vibrating strings of energy
Understanding the key elements of string theory
Hoping to explain the entire universe with string theory
Studying string theory could be the driving scientific goal of the 21st century
String theory is a work in progress, so trying to pin down exactly what
string theory is, or what the fundamental elements are, can be kind of
tricky. Regardless, that's exactly what I try to do in this chapter.
In this chapter, you gain a basic understanding of string theory. I outline the
key elements of string theory, which provide the foundation for most of this
book. I also discuss the possibility that string theory could be the starting
point for a "theory of everything," which would define all of our universe's
physical laws in one simple (or not so simple) mathematical formula. Finally,
I look at the reasons why you should care about string theory.
String Theory: Seeing What Vibrating
Strings Can Tett Us about the Universe
String theory is a physics theory that the universe is composed of vibrating fil-
aments of energy, expressed in precise mathematical language. These strings
of energy represent the most fundamental aspect of nature. The theory also
predicts other fundamental objects, called branes. All of the matter in our uni-
verse consists of the vibrations of these strings (and branes). One important
result of string theory is that gravity is a natural consequence of the theory,
which is why scientists believe that string theory may hold the answer to
possibly uniting gravity with the other forces that affect matter.
/ (/ Part I: Introducing String Theory _
Let me reiterate something important: String theory is a mathematical theory.
It's based on mathematical equations that can be interpreted in certain ways.
If you've never studied physics before, this may seem odd, but all physical
theories are expressed in the language of mathematics. In this book, I avoid
the mathematics and try to get to the heart of what the theory is telling us
about the physical universe.
At present, no one knows exactly what the final version of string theory will
look like. Scientists have some vague notions about the general elements
that will exist within the theory, but no one has come up with the final equa-
tion that represents all of string theory in our universe, and experiments
haven't yet been able to confirm it (though they haven't successfully refuted
it, either). Physicists have created simplified versions of the equation, but it
doesn't quite describe our universe . . . yet.
Using tiny and huge concepts to
create a theory of everything
String theory is a type of high-energy theoretical physics, practiced largely
by particle physicists. It's a quantum field theory (see the sidebar "What is
quantum field theory?") that describes the particles and forces in our uni-
verse based on the way that special extra dimensions within the theory are
wrapped up into a very small size (a process called compactificatiori). This
is the power of string theory — to use the fundamental strings, and the way
extra dimensions are compactified, to provide a geometric description of all
the particles and forces known to modern physics.
Among the forces needed to be described is, of course, gravity. Because
string theory is a quantum field theory, this means that string theory would
be a quantum theory of gravity, known as quantum gravity. The established
theory of gravity, general relativity, has a fluid, dynamic space-time, and one
aspect of string theory that's still being worked on is getting this sort of a
space-time to emerge out of the theory.
The major achievements of string theory are concepts you can't see, unless
you know how to interpret the physics equations. String theory uses no
experiments that provide new insights, but it has revealed profound math-
ematical relationships within the equations, which lead physicists to believe
that they must be true. These properties and relationships — called by
jargon such as various symmetries and dualities, the cancellation of anoma-
lies, and the explanation of black hole entropy — are described in Chapters
10 and 11.
Chapter 1: So What Is String Theory Anyway? / /
What is quantum field theory?
Physicists use fieldsto describe the things that
don't just have a particular position, but exist at
every pointin space. For example, you canthink
about the temperature in a room as a field —
it may be different near an open window than
near a hot stove, and you could imagine mea-
suring the temperature at every single point in
the room. A field theory, then, is a set of rules
that tell you how some field will behave, such
as how the temperature in the room changes
overtime.
In Chapters 7 and 8, you find out about one of
the most important achievements of the 20th
century: the development of quantum theory.
This refers to principles that lead to seemingly
bizarre physical phenomena, which nonethe-
less seem to occur in the subatomic world.
When you combine these two concepts, you get
quantum field theory: a field theory that obeys
the principles of quantum theory. All modern
particle physics is described by quantum field
theories.
In recent years, there has been much public controversy over string theory,
waged across headlines and the Internet. These issues are addressed in Part
V, but they come down to fundamental questions about how science should
be pursued. String theorists believe that their methods are sound, while the
critics believe that they are, at best, questionable. Time and experimental
evidence will tell which side has made the better argument.
A quick took at where
string theory has been
The theory was originally developed in 1968 as a theory that attempted to
explain the behavior of hadrons (such as protons and neutrons, the particles
that make up an atomic nucleus) inside particle accelerators. Physicists later
realized this theory could also be used to explain some aspects of gravity.
For more than a decade, string theory was abandoned by most physicists,
mainly because it required a large number of extra, unseen dimensions. It
rose to prominence again in the mid-1980s, when physicists were able to
prove it was a mathematically consistent theory.
In the mid-1990s, string theory was updated to become a more complex
theory, called M-theory, which contains more objects than just strings. These
new objects were called branes, and they could have anywhere from zero to
nine dimensions. The earlier string theories (which now also include branes)
were seen as approximations of the more complete M-theory.
/ ^ Part I: Introducing String Theory _
Technically, the modern M-theory is more than the traditional string theory,
but the name "string theory" is still often used for M-theory and its various
offspring theories. (Even the original superstring theories have been shown to
include branes.) My convention in this book is to refer to theories that contain
branes, which are variants of M-theory and the original string theories, using
the term "string theory."
Introducing the Key Elements
of String Theory
Five key ideas are at the heart of string theory and come up again and again.
It's best for you to become familiar with these key concepts right off the bat:
K" String theory predicts that all objects in our universe are composed of
vibrating filaments (and membranes) of energy.
J-" String theory attempts to reconcile general relativity (gravity) with
quantum physics.
i^ String theory provides a way of unifying all the fundamental forces of the
universe.
(-" String theory predicts a new connection (called supersymmetry) between
two fundamentally different types of particles, bosons and fermions.
J-" String theory predicts a number of extra (usually unobservable) dimen-
sions to the universe.
I introduce you to the very basics of these ideas in the following sections.
Strings and branes
When the theory was originally developed in the 1970s, the filaments of
energy in string theory were considered to be 1-dimensional objects: strings.
(One-dimensional indicates that a string has only one dimension, length, as
opposed to say a square, which has both length and height dimensions.)
These strings came in two forms — closed strings and open strings. An open
string has ends that don't touch each other, while a closed string is a loop
with no open end. It was eventually found that these early strings, called
Type I strings, could go through five basic types of interactions, as shown in
Figure 1-1.
_ Chapter 1: So What Is String Theory Anyway? / jf
Figure 1-1:
Type I
strings can
go through
five fun-
damental
interactions,
based on
different
ways of
joining and
splitting.
The interactions are based on a string's ability to have ends join and split
apart. Because the ends of open strings can join together to form closed
strings, you can't construct a string theory without closed strings.
^$HBE# This proved to be important, because the closed strings have properties that
^/^ w\ make physicists believe they might describe gravity! In other words, instead of
IJUl J just being a theory of matter particles, physicists began to realize that string
theory may just be able to explain gravity and the behavior of particles.
Over the years, it was discovered that the theory required objects other
than just strings. These objects can be seen as sheets, or branes. Strings can
attach at one or both ends to these branes. A 2-dimensional brane (called a
2-brane) is shown in Figure 1-2. (See Chapter 11 for more about branes.)
/ (l Part I: Introducing String Theory _
Quantum qratfitq
Modern physics has two basic scientific laws: quantum physics and general
relativity. These two scientific laws represent radically different fields of
study. Quantum physics studies the very smallest objects in nature, while
relativity tends to study nature on the scale of planets, galaxies, and the uni-
verse as a whole. (Obviously, gravity affects small particles too, and relativity
accounts for this as well.) Theories that attempt to unify the two theories
are theories of quantum gravity, and the most promising of all such theories
today is string theory.
The closed strings of string theory (see the preceding section) correspond
to the behavior expected for gravity. Specifically, they have properties that
match the long sought-after graviton, a particle that would carry the force of
gravity between objects.
Quantum gravity is the subject of Chapter 2, where I cover this idea in much
greater depth.
Unification of forces
Hand-in-hand with the question of quantum gravity, string theory attempts
to unify the four forces in the universe — electromagnetic force, the strong
nuclear force, the weak nuclear force, and gravity — together into one uni-
fied theory. In our universe, these fundamental forces appear as four differ-
ent phenomena, but string theorists believe that in the early universe (when
there were incredibly high energy levels) these forces are all described
by strings interacting with each other. (If you've never heard of some of
these forces, don't worry! They're individually discussed in greater detail in
Chapter 2 and throughout Part II.)
_ Chapter 1: So What Is String Theory Anyway? J y
Supersymmetry
All particles in the universe can be divided into two types: bosons and fer-
mions. (These types of particles are explained in more detail in Chapter 8.)
String theory predicts that a type of connection, called supersymmetry, exists
between these two particle types. Under supersymmetry, a fermion must
exist for every boson and a boson for every fermion. Unfortunately, experi-
ments have not yet detected these extra particles.
Supersymmetry is a specific mathematical relationship between certain
elements of physics equations. It was discovered outside of string theory,
although its incorporation into string theory transformed the theory into
supersymmetric string theory (or superstring theory) in the mid-1970s. (See
Chapter 10 for more specifics about supersymmetry.)
One benefit of supersymmetry is that it vastly simplifies string theory's
equations by allowing certain terms to cancel out. Without supersymmetry,
the equations result in physical inconsistencies, such as infinite values and
imaginary energy levels.
Because scientists haven't observed the particles predicted by supersym-
metry, this is still a theoretical assumption. Many physicists believe that the
reason no one has observed the particles is because it takes a lot of energy to
generate them. (Energy is related to mass by Einstein's famous E = mc 2 equa-
tion, so it takes energy to create a particle.) They may have existed in the
early universe, but as the universe cooled off and energy spread out after the
big bang, these particles would have collapsed into the lower-energy states
that we observe today. (We may not think of our current universe as particu-
larly low energy, but compared to the intense heat of the first few moments
after the big bang, it certainly is.)
In other words, the strings vibrating as higher-energy particles lost energy and
transformed from one type of particle (one type of vibration) into another,
lower-energy type of vibration.
Scientists hope that astronomical observations or experiments with particle
accelerators will uncover some of these higher-energy supersymmetric par-
ticles, providing support for this prediction of string theory.
Extra dimensions
Another mathematical result of string theory is that the theory only makes
sense in a world with more than three space dimensions! (Our universe has
three dimensions of space — left/right, up/down, and front/back.) Two pos-
sible explanations currently exist for the location of the extra dimensions:
16
Part I: Introducing String Theory _
Iv* The extra space dimensions (generally six of them) are curled up (com-
pactified, in string theory terminology) to incredibly small sizes, so we
never perceive them.
v We are stuck on a 3-dimensional brane, and the extra dimensions extend
off of it and are inaccessible to us.
A major area of research among string theorists is on mathematical models
of how these extra dimensions could be related to our own. Some of these
recent results have predicted that scientists may soon be able to detect
these extra dimensions (if they exist) in upcoming experiments, because
they may be larger than previously expected. (See Chapter 13 for more about
extra dimensions.)
Understanding the Aim of String Theory
To many, the goal of string theory is to be a "theory of everything" — that
is, to be the single physical theory that, at the most fundamental level,
describes all of physical reality. If successful, string theory could explain
many of the fundamental questions about our universe.
Explaining matter and mass
One of the major goals of current string theory research is to construct a
solution of string theory that contains the particles that actually exist in our
String theory started out as a theory to explain particles, such as hadrons,
as the different higher vibrational modes of a string. In most current formula-
tions of string theory, the matter observed in our universe comes from the
lowest-energy vibrations of strings and branes. (The higher-energy vibrations
represent more energetic particles that don't currently exist in our universe.)
The mass of these fundamental particles comes from the ways that these
string and branes are wrapped in the extra dimensions that are compactified
within the theory, in ways that are rather messy and detailed.
For an example, consider a simplified case where the extra dimensions are
curled up in the shape of a donut (called a torus by mathematicians and phys-
icists), as in Figure 1-3.
_ Chapter 1: So What Is String Theory Anyway? / /
A string has two ways to wrap once around this shape:
Iv* A short loop around the tube, through the middle of the donut
u* A long loop wrapping around the entire length of the donut (like a string
wraps around a yo-yo)
The short loop would be a lighter particle, while the long loop is a heavier par-
ticle. As you wrap strings around the torus-shaped compactified dimensions,
you get new particles with different masses.
One of the major reasons that string theory has caught on is that this idea —
that length translates into mass — is so straightforward and elegant. The com-
pactified dimensions in string theory are much more elaborate than a simple
torus, but they work the same way in principle.
It's even possible (though harder to visualize) for a string to wrap in both
directions simultaneously — which would, again, give yet another particle
with yet another mass. Branes can also wrap around extra dimensions, creat-
ing even more possibilities.
Defining space and time
In many versions of string theory, the extra dimensions of space are compac-
tified into a very tiny size, so they're unobservable to our current technology.
Trying to look at space smaller than this compactified size would provide
results that don't match our understanding of space-time. (As you see in
Chapter 2, the behavior of space-time at these small scales is one of the rea-
sons for a search for quantum gravity.) One of string theory's major obsta-
cles is attempting to figure out how space-time can emerge from the theory.
/ Q Part I: Introducing String Theory _
As a rule, though, string theory is built upon Einstein's notion of space-time
(see Chapter 6). Einstein's theory has three space dimensions and one time
dimension. String theory predicts a few more space dimensions but doesn't
change the fundamental rules of the game all that much, at least at low
energies.
At present, it's unclear whether string theory can make sense of the funda-
mental nature of space and time any more than Einstein did. In string theory,
it's almost as if the space and time dimensions of the universe are a backdrop
to the interactions of strings, with no real meaning on their own.
Some proposals have been developed for how this might be addressed,
mainly focusing on space-time as an emergent phenomenon — that is, the
space-time comes out of the sum total of all the string interactions in a way
that hasn't yet been completely worked out within the theory.
However, these approaches don't meet some physicists' definition, leading
to criticism of the theory. String theory's largest competitor, loop quantum
gravity, uses the quantization of space and time as the starting point of its
own theory, as Chapter 18 explains. Some believe that this will ultimately be
another approach to the same basic theory.
Quantizing gravity
The major accomplishment of string theory, if it's successful, will be to show
that it's a quantum theory of gravity. The current theory of gravity, general
relativity, doesn't allow for the results of quantum physics. Because quantum
physics places limitations on the behavior of small objects, it creates major
inconsistencies when trying to examine the universe at extremely small
scales. (See Chapter 7 for more on quantum physics.)
Unifying forces
Currently, four fundamental forces (more precisely called "interactions"
among physicists) are known to physics: gravity, electromagnetic force, weak
nuclear force, and strong nuclear force. String theory creates a framework in
which all four of these interactions were once a part of the same unified force
of the universe.
Under this theory, as the early universe cooled off after the big bang, this uni-
fied force began to break apart into the different forces we experience today.
Experiments at high energies may someday allow us to detect the unification
of these forces, although such experiments are well outside of our current
realm of technology.
_ Chapter 1: So What Is String Theory Anyway? / y
Appreciating the Theory's Amazing
(and Controversial) Implications
Although string theory is fascinating in its own right, what may prove to be
even more intriguing are the possibilities that result from it. These topics are
explored in greater depth throughout the book and are the focus of Parts III
and IV.
Landscape of possible theories
One of the most unexpected and disturbing discoveries of string theory is
that instead of one single theory, it turns out there may be a huge number
of possible theories (or, more precisely, possible solutions to the theory) —
possibly as many as 10 500 different solutions! (That's a 1 followed by 500
zeroes!) While this huge number has prompted a crisis among some string
theorists, others have embraced this as a virtue, claiming that this means
that string theory is very rich. In order to wrap their minds around so many
possible theories, some string theorists have turned toward the anthropic
principle, which tries to explain properties of our universe as a result of our
presence in it. Still others have no problem with this vast number, actually
having expected it and, instead of trying to explain it, just trying to measure
the solution that applies to our universe.
With such a large number of theories available, the anthropic principle allows
a physicist to use the fact that we're here to choose among only those theo-
ries that have physical parameters that allow us to be here. In other words,
our very presence dictates the choice of physical law — or is it merely that
our presence is an observable piece of data, like the speed of light?
The use of the anthropic principle is one of the most controversial aspects
of modern string theory. Even some of the strongest string theory support-
ers have expressed concern over its application, because of the sordid (and
somewhat unscientific) applications to which it has been used in the past and
their feeling that all that is needed is an observation of our universe, without
anything anthropic applied at all.
As anthropic principle skeptics are quick to point out, physicists only adopt
the anthropic principle when they have no other options, and they abandon
it if something better comes along. It remains to be seen if string theorists
will find another way to maneuver through the string theory landscape.
(Chapter 11 has more details about the anthropic principle.)
4m\} Part I: Introducing String Theory _
Parallel universes
Some interpretations of string theory predict that our universe is not the only
one. In fact, in the most extreme versions of the theory, an infinite number
of other universes exist, some of which contain exact duplicates of our own
universe.
As wild as this theory is, it's predicted by current research studying the very
nature of the cosmos itself. In fact, parallel universes aren't just predicted by
string theory — one view of quantum physics has suggested the theoretical
existence of a certain type of parallel universe for more than half a century.
In Chapter 15, 1 explore the scientific concept of parallel universes in greater
detail.
Wormholes
Einstein's theory of relativity predicts warped space called a wormhole (also
called an Einstein-Rosen bridge). In this case, two distant regions of space are
connected by a shorter wormhole, which gives a shortcut between those two
distant regions, as shown in Figure 1-4.
String theory allows for the possibility that wormholes extend not only
between distant regions of our own universe, but also between distant
regions of parallel universes. Perhaps universes that have different physical
laws could even be connected by wormholes. (Chapters 15 and 16 contain
more info on wormholes.)
In fact, it's not clear whether wormholes will exist within string theory at all.
As a quantum gravity theory, it's possible that the general relativity solutions
that give rise to potential wormholes might go away.
_ Chapter 1: So What Is String Theory Anyway? 2 7
The universe as a hologram
In the mid-1990s, two physicists came up with an idea called the holographic
principle. In this theory, if you have a volume of space, you can take all the
information contained in that space and show that it corresponds to infor-
mation "written" on the surface of the space. As odd as it seems, this holo-
graphic principle may be key in resolving a major mystery of black holes that
has existed for more than 20 years!
Many physicists believe that the holographic principle will be one of the
fundamental physical principles that will allow insights into a greater under-
standing of string theory. (Check out Chapter 1 1 for more on the holographic
principle.)
Time traOet
Some physicists believe that string theory may allow for multiple dimen-
sions of time (by no means the dominant view). As our understanding of
time grows with string theory, it's possible that scientists may discover new
means of traveling through the time dimension or show that such theoreti-
cal possibilities are, in fact, impossible, as most physicists believe. (Flip to
Chapter 16 if you're ready to make your time travel reservation.)
The biq banq
String theory is being applied to cosmology, which means that it may give us
insights into the formation of the universe. The exact implications are still
being explored, but some believe that string theory supports the current cos-
mological model of inflation, while others believe it allows for entirely univer-
sal creation scenarios.
Inflation theory predicts that, very shortly after the original big bang, the uni-
verse began to undergo a period of rapid, exponential inflation. This theory,
which applies principles of particle physics to the early universe as a whole,
is seen by many as the only way to explain some properties of the early
universe.
In string theory, there also exists a possible alternate model to our current
big bang model in which two branes collided together and our universe is the
result. In this model, called the ekpyrotic universe, the universe goes through
cycles of creation and destruction, over and over. (Chapter 14 covers the big
bang theory and the ekpyrotic universe.)
4m 2 P art ' : Introducing String Theory _
The end of the universe
The ultimate fate of the universe is a question that physics has long explored,
and a final version of string theory may help us ultimately determine the
matter density and cosmological constant of the universe. By determining
these values, cosmologists will be able to determine whether our universe
will ultimately contract in upon itself, ending in a big crunch — and perhaps
start all over again. (See Chapter 14 for more on these speculations.)
Why Is String Theory So Important)
String theory yields many fascinating subjects for thought, but you may be
wondering about the practical importance of it. For one thing, string theory is
the next step in our growing understanding of the universe. If that's not prac-
tical enough, then there's this consideration: Your tax money goes to fund
scientific research, and the people trying to get that money want to use it to
study string theory (or its alternatives).
A completely honest string theorist would be forced to say that there are
probably no practical applications for string theory, at least in the foresee-
able future. This doesn't look that great on either the cover of a book or a
magazine column, so it gets spiced up with talk about parallel universes,
extra time dimensions, and discovering new fundamental symmetries of
nature. They might exist, but the theory's predictions make it so that they're
unlikely to ever be particularly useful, so far as we know.
Understanding the nature of the universe better is a good goal in its own
right — as old as humanity, some might say — but when you're looking
at funding multibillion dollar particle accelerators or research satellite
programs, you might want something tangible for your money and, unfor-
tunately, there's no reason to think that string theory is going to give you
anything practical.
Does this mean that exploring string theory isn't important? No, and it's my
hope that reading Part II of this book will help illuminate the key at the heart
of the search for string theory, or any new scientific truth.
No one knows where a scientific theory will lead until the theory is developed
and tested.
In 1905, when Albert Einstein first presented his famous equation E = mc 2 , he
thought it was an intriguing relationship but had no idea that it would result
in something as potent as the atomic bomb. He had no way of knowing the
_ Chapter 1: So What Is String Theory Anyway? 23
corrections to time calculations demanded by special relativity and general
relativity would someday be required to get the worldwide global positioning
system (GPS) to operate correctly (as discussed in Chapter 6).
Quantum physics, which on the surface is about as theoretical of a study as
they come, is the basis for the laser and transistor, two pieces of technology
that are at the heart of modern computers and communication systems.
Even though we don't know what a purely theoretical concept like string
theory may lead to, history has shown that it will almost certainly lead some-
where profound.
For an example of the unexpected nature of scientific progress, consider the
discovery and study of electricity, which was originally seen as a mere parlor
trick. You could predict some technologies from the discovery of electricity,
to be sure, such as the light bulb. But some of the most profound discoveries
are things that may never have been predicted — radio and television, the
computer, the Internet, the cellphone, and so on.
The impact of science extends into culture as well. Another byproduct of
electricity is rock and roll music, which was created with the advent of elec-
tric guitars and other electric musical instruments.
If electricity can lead to rock and roll and the Internet, then imagine what sort
of unpredicted (and potentially unpredictable) cultural and technological
advances string theory could lead to!
4*11 Part I: Introducing String Theory _
Chapter 2
The Physics Road Dead Ends
at Quantum Gravity
In This Chapter
Squaring off: Gravity and quantum physics just don't get along
Seeing four types of particle interactions
Hoping to tie all of physics into one equation with quantum gravity
V)
#«^hysicists like to group concepts together into neat little boxes with
w labels, but sometimes the theories they try to put together just don't
want to get along. Right now, nature's fundamental physical laws can fit into
one of two boxes: general relativity or quantum physics. But concepts from
one box just don't work together well with concepts from the other box.
Any theory that can get these two physics concepts to work together would
be called a theory of quantum gravity. String theory is currently the most likely
candidate for a successful theory of quantum gravity.
In this chapter, I explain why scientists want (and need) a theory of quan-
tum gravity. I begin by giving an overview of the scientific understanding of
gravity, which is defined by Einstein's theory of general relativity, and our
understanding of matter and the other forces of nature, in terms of quantum
mechanics. With these fundamental tools in place, I then explain the ways in
which these two theories clash with each other that provides the basis for
quantum gravity. Finally, I outline various attempts to unify these theories
and the forces of physics together into one coherent system, and the failures
they've run into.
26
Part I: Introducing String Theory _
Understanding Tu/o Schools
of Thought on Gravity
Physicists are searching for a theory of quantum gravity because the current
laws governing gravity don't work in all situations. Specifically, the theory
of gravity seems to "break down" (that is, the equations become physically
meaningless) in certain circumstances that I describe later in the chapter.
To understand what this means, you must first understand a bit about what
physicists know about gravity.
Gravity is an attractive force that binds objects together, seemingly across
any amount of distance. The formulation of the classical theory of gravity
by Sir Isaac Newton was one of the greatest achievements of physics. Two
centuries later, the reinvention of gravity by Albert Einstein placed him in the
pantheon of indisputably great scientific thinkers of all time.
Unless you're a physicist, you probably take gravity for granted. It's an amaz-
ing force, able to hold the heavens together while being overcome by my
3-year-old when he's on a swing — but not for long. At the scale of an atom,
gravity is irrelevant compared to the electromagnetic force. In fact, a simple
magnet can overcome the entire force of the planet Earth to pick up metallic
objects, from paper clips to automobiles.
Aleutton's taW of gravity: Gravity as force
Sir Isaac Newton developed his theory of gravity in the late 1600s. This amaz-
ing theory involved bringing together an understanding of astronomy and the
principles of motion (known as mechanics or kinematics) into one compre-
hensive framework that also required the invention of a new form of mathe-
matics: calculus. In Newton's gravitational theory, objects are drawn together
by a physical force that spans vast distances of space.
The key is that gravity binds all objects together (much like the Force in Star
Wars). The apple falling from a tree and the moon's motion around Earth are
two manifestations of the exact same fundamental force.
The relationship that Newton discovered was a mathematical relationship
(he did, after all, have to invent calculus to get it all to work out), just like
relativity, quantum mechanics, and string theory.
In Newton's gravitational theory, the force between two objects is based on
the product of their masses, divided by the square of the distance between
them. In other words, the heavier the two objects are, the more force there is
between them, assuming the distance between them stays the same. (See the
nearby sidebar "A matter of mass" for clarification of this relationship.)
_ Chapter 2: The Physics Road Dead Ends at Quantum Gravity J? /
A matter of mass
When I say that the force between objects is
proportional to the mass of the two objects, you
may think this means that heavier things fall
fasterthan lighterthings. For example, wouldn't
a bowling ball fall fasterthan a soccer ball?
In fact, as Galileo showed (though not with
modern bowling and soccer balls) years before
Newton was born, this isn't the case. For cen-
turies, most people had assumed that heavier
objects fell faster than light objects. Newton
was aware of Galileo's results, which was why
he was able to figure out how to define force
the way he did.
By Newton's explanation, it takes more force to
move a heavier object. If you dropped a bowl-
ing ball and soccer ball off a building (which I
don't recommend), they would accelerate at
the exactsame rate (ignoring air resistance) —
approximately 9.8 meters per second.
The force acting between the bowling ball and
Earth would be higher than the force acting on
the soccer ball, but because it takes more force
to get the bowling ball moving, the actual rate of
acceleration between the two is identical.
Realistically, if you performed the experiment
there would be a slight difference. Because
of air resistance, the lighter soccer ball would
probably be slowed down if dropped from a
high enough point, while the bowling ball would
not. But a properly constructed experiment, in
which air resistance is completely neutralized
(such as in a vacuum), shows that the objects
fall at the same rate, regardless of mass.
The fact that the force is divided by distance squared means that if the same
two objects are closer to each other, the power of gravity increases. If the dis-
tance gets wider, the force drops. The inverse square relationship means that
if the distance doubles, the force drops to one-fourth of its original intensity. If
the distance is halved, the force increases by four times.
If the objects are very far away, the effect of gravity becomes very small. The
reason gravity has any impact on the universe is because there's a lot of it.
Gravity itself is very weak, as forces go.
^jABE# The opposite is true, as well, and if two objects get extremely close to each
other — and I'm talking extremely close here — then gravity can become
incredibly powerful, even among objects that don't have much mass, like the
fundamental particles of physics.
This isn't the only reason gravity is observed so much. Gravity's strength in the
universe also comes from the fact that it's always attracting objects together.
The electromagnetic force sometimes attracts objects and sometimes repulses
them, so on the scale of the universe at large, it tends to counteract itself.
Finally, gravity interacts at very large distances, as opposed to some other
forces (the nuclear forces) that only work at distances smaller than an atom.
I delve a bit deeper into Newton's work, both in gravity and in other related
areas, in Chapter 5.
4mO ' >art ' : Introducing String Theory _
Despite the success of Newton's theory, he had a few nagging problems
in the back of his mind. First and foremost among those was the fact that
though he had a model for gravity, he didn't know why gravity worked. The
gravity that he described was an almost mystical force (like the Force!),
acting across great distances with no real physical connection required. It
would take two centuries and Albert Einstein to resolve this problem.
Einstein's taW of gravity:
Gravity as geometry
Albert Einstein would revolutionize the way physicists saw gravity. Instead
of gravity as a force acting between objects, Einstein instead envisioned a
universe in which each object's mass caused a slight bending of space (actu-
ally space-time) around it. The movement of an object along the shortest
distance in this space-time was gravity. Instead of being a force, gravity was
actually an effect of the geometry of space-time itself.
Einstein proposed that motion in the universe could be explained in terms
of a coordinate system with three space dimensions — up/down, left/right,
and backward/forward, for example — and one time dimension. This
4-dimensional coordinate system, developed by Einstein's old professor
Hermann Minkowski, was called space-time, and came out of Einstein's
1905 theory of special relativity.
As Einstein generalized this theory, creating the theory of general relativity in
1916, he was able to include gravity in his explanations of motion. In fact, the
concept of space-time was crucial to it. The space-time coordinate system
bent when matter was placed in it. As objects moved within space and time,
they naturally tried to take the shortest path through the bent space-time.
We follow our orbit around the sun because it's the shortest path (called a
geodesic in mathematics) through the curved space-time around the sun.
Einstein's relativity is covered in depth in Chapter 6, and the major implica-
tions of relativity to the evolution of the universe are covered in Chapter 9.
The space-time dimensions are discussed in Chapter 13.
Describing Matter: Physical
and Eneryy-Filled
Einstein helped to revolutionize our ideas about the composition of matter as
much as he did about space, time, and gravity. Thanks to Einstein, scientists
_ Chapter 2: The Physics Road Dead Ends at Quantum Gravity 2 y
realize that mass — and therefore matter itself — is a form of energy. This
realization is at the heart of modern physics. Because gravity is an interac-
tion between objects made up of matter, understanding matter is crucial to
understanding why physicists need a theory of quantum gravity.
Viewing matter classically:
Chunks of stuff
The study of matter is one of the oldest physics disciplines, because phi-
losophers tried to understand what made up objects. Even fairly recently, a
physical understanding of matter was elusive, as physicists debated the exis-
tence of atoms — tiny, indivisible chunks of matter that couldn't be broken
up anymore.
One key physics principle was that matter could be neither created nor
destroyed, but could only change from one form to another. This principle is
known as the conservation of mass.
Though it can't be created or destroyed, matter can be broken, which led to
the question of whether there was a smallest chunk of matter, the atom, as
the ancient Greeks had proposed — a question that, throughout the 1800s,
seemed to point toward an affirmative answer.
As an understanding of thermodynamics — the study of heat and energy,
which made things like the steam engine (and the Industrial Revolution)
possible — grew, physicists began to realize that heat could be explained
as the motion of tiny particles.
The atom had returned, though the findings of 20th-century quantum physics
would reveal that the atom wasn't indivisible as everyone thought.
Viewing matter at a quantum
scale: Chunks of energy
With the rise of modern physics in the 20th century, two key facts about
matter became clear:
Iu* As Einstein had proposed with his famous E = mc 2 equation, matter and
energy are, in a sense, interchangeable.
J-" Matter was incredibly complex, made up of an array of bizarre and
unexpected types of particles that joined together to form other types
of particles.
3 v P art ' : Introducing String Theory _
jftBE# The atom, it turned out, was composed of a nucleus surrounded by electrons.
The nucleus was made up of protons and neutrons, which were, in turn, made
iMJj ) up of strange new particles called quarks! As soon as physicists thought they
had reached a fundamental unit of matter, they seemed to discover that it
could be broken open and still smaller units could be pulled out.
Not only that, but even these fundamental particles didn't seem to be
enough. It turned out that there were three families of particles, some of
which only appeared at significantly higher energies than scientists had pre-
viously explored.
Today, the Standard Model of particle physics contains 18 distinct fundamen-
tal particles, 17 of which have been observed experimentally. (Physicists are
still waiting on the Higgs boson.)
Grasping for the Fundamental
Farces of Physics
Even while the numbers of particles became more bizarre and complex, the
ways those objects interacted turned out to be surprisingly straightforward.
In the 20th century, scientists discovered that objects in the universe experi-
enced only four fundamental types of interactions:
IJ-" Electromagnetism
(-" Strong nuclear force
W Weak nuclear force
v* Gravity
Physicists have discovered profound connections between these forces —
except for gravity, which seems to stand apart from the others for reasons
that physicists still aren't completely certain about. Trying to incorporate
gravity with all the other forces — to discover how the fundamental forces
are related to each other — is a key insight that many physicists hope a
theory of quantum gravity will offer.
Electromagnetism: Super-speedy
energy WaOes
Discovered in the 19th century, the electromagnetic force (or electromag-
netism) is a unification of the electrostatic force and the magnetic force. In
the mid-20th century, this force was explained in a framework of quantum
_ Chapter 2: The Physics Road Dead Ends at Quantum Gravity j /
mechanics called quantum electrodynamics, or QED. In this framework, the
electromagnetic force is transferred by particles of light, called photons.
The relationship between electricity and magnetism is covered in Chapter 5,
but the basic relationship comes down to electrical charge and its motion.
The electrostatic force causes charges to exert forces on each other in a
relationship that's similar to (but more powerful than) gravity — an inverse
square law. This time, though, the intensity is based not on the mass of the
objects, but the charge.
The electron is a particle that contains a negative electrical charge, while the
proton in the atomic nucleus has a positive electrical charge. Traditionally,
electricity is seen as the flow of electrons (negative charge) through a wire.
This flow of electrons is called an electric current.
A wire with an electrical current flowing through it creates a magnetic field.
Alternately, when a magnet is moved near a wire, it causes a current to flow.
(This is the basis of most electric power generators.)
This is the way in which electricity and magnetism are related. In the 1800s,
physicist James Clerk Maxwell unified the two concepts into one theory,
called electromagnetism, which depicted this force as waves of energy moving
through space.
One key component of Maxwell's unification was a discovery that the elec-
tromagnetic force moved at the speed of light. In other words, the electro-
magnetic waves that Maxwell predicted from his theory were a form of light
waves.
Quantum electrodynamics retains this relationship between electromagne-
tism and light, because in QED the information about the force is transferred
between two charged particles (or magnetic particles) by another particle —
a photon, or particle of light. (Physicists say that the electromagnetic force is
mediated by a photon.)
Nuclear forces: What the strong force
joins, the Weak force tears apart
In addition to gravity and electromagnetism, 20th-century physics discovered
two nuclear forces called the strong nuclear force and weak nuclear force.
These forces are also mediated by particles. The strong force is mediated
by a type of particle called a gluon. The weak force is mediated by three
particles: Z, W*, and W~ bosons. (You can read more about these particles in
Chapter 8.)
3^- ^ art '" '"Educing String Theory _
The strong nuclear force holds quarks together to form protons and neu-
trons, but it also holds the protons and neutrons together inside the atom's
nucleus.
The weak nuclear force, on the other hand, is responsible for radioactive
decay, such as when the neutron decays into a proton. The processes gov-
erned by the weak nuclear force are responsible for the burning of stars and
the formation of heavy elements inside of stars.
Infinities: Why Einstein and
the Quanta Don't Get Atony
Einstein's theory of general relativity, which explains gravity, does an excel-
lent job at explaining the universe on the scale of the cosmos. Quantum phys-
ics does an excellent job of explaining the universe on the scale of an atom or
smaller. In between those scales, good old-fashioned classical physics usually
rules.
Unfortunately, some problems bring general relativity and quantum physics
into conflict, resulting in mathematical infinities in the equations. (Infinity
is essentially an abstract number that is larger than any other numbers.
Though certain cartoon characters like to go "To infinity and beyond," scien-
tists don't like to see infinities come up in mathematical equations.) Infinities
come up in quantum physics, but physicists have developed mathemati-
cal techniques to tame them in many of those cases, so the results match
experiments. In some cases, however, these techniques don't apply. Because
physicists never witness real infinities in nature, these troublesome problems
motivate a search for quantum gravity.
Each of the theories works fine on its own, but when you get into areas where
both have something specific to say about the same thing — such as what's
going on at the border of a black hole — things get very complicated. The
quantum fluctuations make the distinction between the inside and outside of
the black hole kind of fuzzy, and general relativity needs that distinction to
work properly. Neither theory by itself can fully explain what's going on in
these specific cases.
This is the heart of why physicists need a theory of quantum gravity. With
the current theories, you get situations that don't look like they make sense.
Physicists don't see infinities, yet as you'll see, both relativity and quantum
physics indicate that they should exist. Reconciling this bizarre region in the
middle, where neither theory can fully describe what's going on, is the goal of
quantum gravity.
_ Chapter 2: The Physics Road Dead Ends at Quantum Gravity 33
^JVBEfl-
Singularities: Bendinq qraVitq
to the breaking point
Because matter causes a bending of space-time, cramming a lot of matter into
a very small space causes a lot of bending of space-time. In fact, some solu-
tions to Einstein's general relativity equations show situations where space-
time bends an infinite amount — called a singularity. Specifically, a space-time
singularity shows up in the mathematical equations of general relativity in
two situations:
IJ-" During the early big bang period of the universe's history
v* Inside black holes
These subjects are covered in more detail in Chapter 9, but both situations
involve a density of matter (a lot of matter in a small space) that's enough
to cause problems with the smooth space-time geometry that relativity
depends on.
These singularities represent points where the theory of general relativ-
ity breaks down completely. Even talking about what goes on at this point
becomes meaningless, so physicists need to refine the theory of gravity to
include rules about how to talk about these situations in a meaningful way.
Some believe that this problem can be solved by altering Einstein's theory
of gravity (as you see in Chapter 19). String theorists don't usually want to
modify gravity (at least at the energy levels scientists normally look at); they
just want to create a framework that allows gravity to work without running
into these mathematical (and physical) infinities.
Quantum jitters: Space-time under
a Quantum microscope
A second type of infinity, proposed by John Wheeler in 1955, is the quantum
foam or, as it's called by string theorist and best-selling author Brian Greene,
the quantum jitters. Quantum effects mean that space-time at very tiny dis-
tance scales (called the Planck length) is a chaotic sea of virtual particles
being created and destroyed. At these levels, space-time is certainly not
smooth as relativity suggests, but is a tangled web of extreme and random
energy fluctuations, as shown in Figure 2-1.
jU Part I: Introducing String Theory _
Figure 2-1:
If you
zoom in on
space-time
enough,
a chaotic
"quantum
foam"
may exist.
The basis for the quantum jitters is the uncertainty principle, one of the key
(and most unusual) features of quantum physics. This is explained in more
detail in Chapter 7, but the key component of the uncertainty principle is that
certain pairs of quantities — for example, position and velocity, or time and
energy — are linked together, so that the more precisely one is measured,
the more uncertain the other quantity is. This isn't just a statement about
measurement, though, but a fundamental uncertainty in nature!
In other words, nature is a bit "blurry" according to quantum physics. This
blurriness only shows up at very small distances, but this problem creates the
quantum foam.
One example of the blurriness comes in the form of virtual particles.
According to quantum field theory (a field theory is one where each point in
space has a certain value, similar to a gravitational field or electromagnetic
field), even the empty void of space has a slight energy associated with it.
This energy can be used to, very briefly, bring a pair of particles — a particle
and its antiparticle, to be precise — into existence. The particles exist for
only a moment, and then destroy each other. It's as if they borrowed enough
energy from the universe to exist for just a few fractions of a second.
The problem is that when you look at space-time at very small scales, the
effects of these virtual particles become very important. The energy fluctua-
tions predicted by the uncertainty principle take on massive proportions.
Without a quantum theory of gravity, there's no way to really figure out
what's going on at sizes that small.
_ Chapter 2: The Physics Road Dead Ends at Quantum Gravity y f}
Unifying the Farces
The attempt to unite gravity with the other three forces, as well as with quan-
tum physics, was one of the driving forces of physics throughout the 20th
century (and it still is). In a way, these sorts of unifications of different ideas
are the major discoveries in science throughout the ages.
Quantum electrodynamics successfully created a quantum theory of electro-
magnetism. Later, the electroweak theory unified this theory together with
the weak nuclear force. The strong nuclear force is explained by quantum
chromodynamics. The current model of physics that explains all three of
these forces is called the Standard Model of particle physics, which is cov-
ered in much more detail in Chapter 8. Unifying gravity with the other forces
would create a new version of the Standard Model and would explain how
gravity works on the quantum level. Many physicists hope that string theory
will ultimately prove to be this theory.
Einstein's failed quest to
explain everything
After Einstein successfully worked the major kinks out of his theory of gen-
eral relativity, he turned his attention toward trying to unify this theory of
gravity with electromagnetism, as well as with quantum physics. In fact,
Einstein would spend most of the rest of his life trying to develop this unified
theory, but would die unsuccessful.
Throughout the quest, Einstein looked at almost any theory he could think
of. One of these ideas was to add an extra space dimension and roll it up into
a very small size. This approach, called a Kaluza-Klein theory after the men
who created it, is addressed in Chapter 6. This same approach would eventu-
ally be used by string theorists to deal with the pesky extra dimensions that
arose in their own theories.
Ultimately, none of Einstein's attempts bore fruit. To the day of his death,
he worked feverishly on completing his unified field theory in a manner that
many physicists have considered a sad end to such a great career.
Today, however, some of the most intense theoretical physics work is in the
search for a theory to unify gravity and the rest of physics, mainly in the form
of string theory.
3 v P art ' : Introducing String Theory _
A particle of gravity: The qraOiton
The Standard Model of particle physics explains electromagnetism, the
strong nuclear force, and the weak nuclear force as fields that follow the
rules of gauge theory. Gauge theory is based heavily on mathematical sym-
metries. Because these forces are quantum theories, the gauge fields come
in discrete units (that's where the word quantum comes from) — and these
units actually turn out to be particles in their own right, called gauge bosons.
The forces described by a gauge theory are carried, or mediated, by these
gauge bosons. For example, the electromagnetic force is mediated by the
proton. When gravity is written in the form of a gauge theory, the gauge
boson for gravity is called the graviton. (If you're confused about gauge theo-
ries, don't worry too much — just remember that the graviton is what makes
gravity work and you'll know everything that you need to know to under-
stand their application to string theory.)
Physicists have identified some features of the theoretical graviton so that,
if it exists, it can be recognized. For one thing, the particle is massless, which
means it has no rest mass — the particle is always in motion, and that proba-
bly means it travels at the speed of light (although in Chapter 19 you find out
about a theory of modified gravity in which gravity and light move through
space at different speeds).
Another feature of the graviton is that it has a spin of 2. (Spin is a quantum
number indicating an inherent property of a particle that acts kind of like
angular momentum. Fundamental particles have an inherent spin, meaning
that they interact with other particles like they're spinning even when they
aren't.)
A graviton also has no electrical charge. It's a stable particle, which means it
would not decay.
So physicists are looking for a massless particle moving at an incredibly fast
speed, with no electrical charge, and a quantum spin of 2. Even though the
graviton has never been discovered by experiment, it's the gauge boson that
mediates the gravitational force. Given the incredibly weak strength of gravity in
relation to other forces, trying to identify gravitons is an incredibly hard task.
_ Chapter 2: The Physics Road Dead Ends at Quantum Gravity j /
The possible existence of the graviton in string theory is one of the major
motivations for looking toward the theory as a likely solution to the problem
of quantum gravity.
Supersymmetry's role in quantum gravity
Supersymmetry is a principle that says that two types of fundamental par-
ticles, bosons and fermions, are connected to each other. The benefit of this
type of symmetry is that the mathematical relationships in gauge theory
reduce in such a way that unifying all the forces becomes more feasible. (I
explain bosons and fermions in greater detail in Chapter 8, while I present a
more detailed discussion of supersymmetry in Chapter 10.)
The top graph in Figure 2-2 shows the three forces described by the Standard
Model modeled at different energy levels. If the three forces met up in the
same point, it would indicate that there might be an energy level where these
three forces became fully unified into one superforce.
However, as seen in the lower graph of Figure 2-2, when supersymmetry is
introduced into the equation (literally, not just metaphorically), the three
forces meet in a single point. If supersymmetry proves to be true, it's strong
evidence that the three forces of the Standard Model unify at high enough
energy.
Many physicists believe that all four forces were once unified at high energy
levels, but as the universe reduced into a lower-energy state, the inherent
symmetry between the forces began to break down. This broken symmetry
caused the creation of four distinct forces of nature.
The goal of a theory of quantum gravity is, in a sense, an attempt to look
back in time, to when these four forces were unified as one. If successful, it
would profoundly affect our understanding of the first few moments of the
universe — the last time that the forces joined together in this way.
3© Part I: Introducing String Theory
Standard Model
\ strong
0.08 -
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electromagnetic
P
Energy/GeV
0.12 \r~^ ' ' ' ' "~
Minimal Supersymmetric Standard Model
Figure 2-2: | 008 |~ stron 9
If super- ^
symmetry is ~
added, the co
forces in the js 0.04 I weak
Standard —
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become electromagnetic
0.00 I L
high enough 10 4 10 s 10' 2
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^^^^^ Energy/GeV
10 20
Chapter 3
Accomplishments and Failures
of String Theory
In This Chapter
Embracing string theory's achievements
Poking holes in string theory
Wondering what the future of string theory holds
c
^^tring theory is a work in progress, having captured the hearts and minds
^^of much of the theoretical physics community while being apparently
disconnected from any realistic chance of definitive experimental proof.
Despite this, it has had some successes — unexpected predictions and
achievements that may well indicate string theorists are on the right track.
String theory critics would also point out (and many string theorists would
probably agree) that the last decade hasn't been kind to string theory
because the momentum toward a unified theory of everything has slowed
because of a fracture among many different versions of string theory, instead
of a single version of the theory.
In this chapter, you see some of the major successes and failures of string
theory, as well as look at the possibilities for where string theory may go
from here. The controversy over string theory rests entirely on how much
significance physicists give to these different outcomes.
Celebrating String Theory's Successes
String theory has gone through many transformations since its origins in
1968 when it was hoped to be a model of certain types of particle collisions.
It initially failed at that goal, but in the 40 years since, string theory has
developed into the primary candidate for a theory of quantum gravity. It has
driven major developments in mathematics, and theorists have used insights
(l (/ Part I: Introducing String Theory _
from string theory to tackle other, unexpected problems in physics. In fact,
the very presence of gravity within string theory is an unexpected outcome!
Predicting gravity out of strings
The first and foremost success of string theory is the unexpected discovery
of objects within the theory that match the properties of the graviton. These
objects are a specific type of closed strings that are also massless particles
that have spin of 2, exactly like gravitons. To put it another way, gravitons
are a spin-2 massless particle that, under string theory, can be formed by a
certain type of vibrating closed string. String theory wasn't created to have
gravitons — they're a natural and required consequence of the theory.
One of the greatest problems in modern theoretical physics is that grav-
ity seems to be disconnected from all the other forces of physics that are
explained by the Standard Model of particle physics. String theory solves this
problem because it not only includes gravity, but it makes gravity a neces-
sary byproduct of the theory.
Explaining what happens
to a black hole (sort of)
A major motivating factor for the search for a theory of quantum gravity is
to explain the behavior of black holes, and string theory appears to be one
of the best methods of achieving that goal. String theorists have created
mathematical models of black holes that appear similar to predictions made
by Stephen Hawking more than 30 years ago and may be at the heart of
resolving a long-standing puzzle within theoretical physics: What happens to
matter that falls into a black hole?
Scientists' understanding of black holes has always run into problems,
because to study the quantum behavior of a black hole you need to some-
how describe all the quantum states (possible configurations, as defined by
quantum physics) of the black hole. Unfortunately, black holes are objects in
general relativity, so it's not clear how to define these quantum states. (See
Chapter 2 for an explanation of the conflicts between general relativity and
quantum physics.)
.jjjflBEfl String theorists have created models that appear to be identical to black holes
' /^"bN in certain simplified conditions, and they use that information to calculate the
|Mjj J quantum states of the black holes. Their results have been shown to match
Hawking's predictions, which he made without any precise way to count the
quantum states of the black hole.
_ Chapter 3: Accomplishments and Failures of String Theory (l /
This is the closest that string theory has come to an experimental prediction.
Unfortunately, there's nothing experimental about it because scientists can't
directly observe black holes (yet). It's a theoretical prediction that unexpect-
edly matches another (well-accepted) theoretical prediction about black
holes. And, beyond that, the prediction only holds for certain types of black
holes and has not yet been successfully extended to all black holes.
For a more extended look at black holes and string theory, check out
Chapters 9, 11, and 14.
Explaining quantum field theory
using string theory
One of the major successes of string theory is something called the
Maldacena conjecture, or the AdS/CFT correspondence. (I get into what this
stands for and means in Chapter 11.) Developed in 1997 and soon expanded
on, this correspondence appears to give insights into gauge theories, such as
those at the heart of quantum field theory. (See Chapter 2 for an explanation
of gauge theories.)
The original AdS/CFT correspondence, written by Juan Maldacena, proposes
that a certain 3-dimensional (three space dimensions, like our universe)
gauge theory, with the most supersymmetry allowed, describes the same
physics as a string theory in a 4-dimensional (four space dimensions) world.
This means that questions about string theory can be asked in the language
of gauge theory, which is a quantum theory that physicists know how to
work with!
Like John TraOotta, string theory
keeps making a comeback
String theory has suffered more setbacks than probably any other scientific
theory in the history of the world, but those hiccups don't seem to last that
long. Every time it seems that some flaw comes along in the theory, the math-
ematical resiliency of string theory seems to not only save it, but to bring it
back stronger than ever.
When extra dimensions came into the theory in the 1970s, the theory was
abandoned by many, but it had a comeback in the first superstring revolu-
tion. It then turned out there were five distinct versions of string theory,
but a second superstring revolution was sparked by unifying them. When
string theorists realized a vast number of solutions of string theories (each
solution to string theory is called a vacuum, while many solutions are called
[l £ Part I: Introducing String Theory _
vacua) were possible, they turned this into a virtue instead of a drawback.
Unfortunately, even today, some scientists believe that string theory is failing
at its goals. (See "Considering String Theory's Setbacks" later in this chapter.)
Being the most popular theory in town
Many young physicists feel that string theory, as the primary theory of quan-
tum gravity, is the best (or only) avenue for making a significant contribution
to our understanding of this topic. Over the last two decades, high-energy
theoretical physics (especially in the United States) has become dominated
by string theorists. In the high-stakes world of "publish or perish" academia,
this is a major success.
Why do so many physicists turn toward this field when it offers no experi-
mental evidence? Some of the brightest theoretical physicists of either the
20th or the 21st centuries — Edward Witten, John Henry Schwarz, Leonard
Susskind, and others you meet throughout this book — continually return to
the same common reasons in support of their interest:
(-" If string theory were wrong, it wouldn't provide the rich structure that it
does, such as with the development of the heterotic string (see Chapter
10) that allows for an approximation of the Standard Model of physics
within string theory.
j-" If string theory were wrong, it wouldn't lead to better understandings
of quantum field theory, quantum chromodynamics (see Chapter 8),
or the quantum states of black holes, as have been presented by the
work of Leonard Susskind, Andrew Strominger, Cumrun Vafa, and Juan
Maldacena (see Chapters 11 and 14).
j-" If string theory were wrong, it would have collapsed in upon itself well
before now, instead of passing many mathematical consistency checks
(such as those discussed in Chapter 10) and providing more and more
elaborate ways to be interpreted, such as the dualities and symmetries
that allowed for the presentation of M-theory (as discussed in Chapter 1 1).
This is how theoretical physicists think, and it's why so many of them
continue to believe that string theory is the place to be. The mathemati-
cal beauty of the theory, the fact that it's so adaptable, is seen as one of its
virtues. The theory continues to be refined, and it hasn't been shown to be
incompatible with our universe. There has been no brick wall where the
theory failed to provide something new and (in some eyes, at least) meaning-
ful, so those studying string theory have had no reason to give up and look
somewhere else. (The history of string theory in Chapters 10 and 11 offers a
better appreciation of these achievements.)
_ Chapter 3: Accomplishments and Failures of String Theory [ly
Whether this resilience of string theory will translate someday into proof that
the theory is fundamentally correct remains to be seen, but for the majority
of those working on the problems, confidence is high.
As you can read in Chapter 17, this popularity is also seen by some critics
as a flaw. Physics thrives on the rigorous debate of conflicting ideas, and
some physicists are concerned that the driving support of string theory, to
the exclusion of all other ideas, isn't healthy for the field. For some of these
critics, the mathematics of string theory has, indeed, already shown that the
theory isn't performing as expected (or, in their view, as needed to be a fun-
damental theory) and the string theorists are in denial.
Considering String Theory's Setbacks
Because string theory has made so few specific predictions, it's hard to dis-
prove it, but the theory has fallen short of some of the hype about how it will
be a fundamental theory to explain all the physics in our universe, a "theory
of everything." This failure to meet that lofty goal seems to be the basis of
many (if not most) of the attacks against it.
In Chapter 17, you find more detailed criticisms of string theory. Some of
these cut to the very heart of whether string theory is even scientific or
whether it's being pursued in the correct way. For now, I leave these more
abstract questions and focus on three issues that even most string theorists
aren't particularly happy about:
v" Because of supersymmetry, string theory requires a large number of
particles beyond what scientists have ever observed.
v" This new theory of gravity was unable to predict the accelerated expan-
sion of the universe that was detected by astronomers.
u* A vastly large number of mathematically feasible string theory vacua
(solutions) currently exist, so it seems virtually impossible to figure out
which could describe our universe.
The following sections cover these dilemmas in more detail.
The universe doesn't haVe enough particles
For the mathematics of string theory to work, physicists have to assume a
symmetry in nature called supersymmetry, which creates a correspondence
between different types of particles. One problem with this is that instead of
the 18 fundamental particles in the Standard Model, supersymmetry requires
at least 36 fundamental particles (which means that nature allows 18 par-
ticles that scientists have never seen!).
li(l Part I: Introducing String Theory _
In some ways, string theory does make things simpler — the fundamental
objects are strings and branes or, as predicted by matrix theory, zero-
dimensional branes called partons. These strings, branes, or possibly partons
make up the particles that physicists have observed (or the ones they hope to
observe). But that's on a very fundamental level; from a practical standpoint,
string theory doubles the number of particles allowed by nature from 18 to 36.
One of the biggest possible successes for string theory would be to experi-
mentally detect these missing supersymmetric partner particles. The hope of
many theoretical physicists is that when the Large Hadron Collider particle
accelerator at CERN in Switzerland goes fully online, it will detect super-
symmetric particles.
Even if successful, proof of supersymmetry doesn't inherently prove string
theory, so the debate would continue to rage on, but at least one major
objection would be removed. Supersymmetry might well end up being true,
whether or not string theory as a whole is shown to accurately describe
nature.
Dark energy: The discovery string
theory should haVe predicted
Astronomers found evidence in 1998 that the expansion of the universe
was actually accelerating. This accelerated expansion is caused by the dark
energy that appears so often in the news. Not only did string theory not pre-
dict the existence of dark energy, but attempts to use science's best theories
to calculate the amount of dark energy comes up with a number that's vastly
larger than the one observed by astronomers. The theory just absolutely
failed to initially make sense of dark energy.
Claiming this as a flaw of string theory is a bit more controversial than the
other two, but there's some (albeit questionable) logic behind it. The goal of
string theory is nothing less than the complete rewriting of gravitational law,
so it's not unreasonable to think that string theory should have anticipated
dark energy in some way. When Einstein constructed his theory of general rela-
tivity, the mathematics indicated that space could be expanding (later proved
to be true). When Paul Dirac formulated a quantum theory of the electron, the
mathematics indicated an antiparticle existed (later proved to actually exist).
A profound theory like string theory can be expected to illuminate new facts
about our universe, not be blind-sided by unanticipated discoveries.
Of course, no other theory anticipated an accelerating expansion of the uni-
verse either. Prior to the observational evidence (some of which is still con-
tested, as you find out in Chapter 19), cosmologists (and string theorists) had
no reason to assume that the expansion rate of space was increasing. Years
_ Chapter 3: Accomplishments and Failures of String Theory (l J
after dark energy was discovered, it was shown that string theory could be
modified to include it, which string theorists count as a success (although
the critics continue to be unsatisfied).
Where did all of these "fundamental"
theories come from}
Unfortunately, as string theorists performed more research, they had a
growing problem (pun intended). Instead of narrowing in on a single vacuum
(solution) that could be used to explain the universe, it began to look like
there were an absurdly large number of vacua. Some physicists' hopes that a
unique, fundamental version of string theory would fall out of the mathemat-
ics effectively dissolved.
In truth, such hype was rarely justified in the first place. In general relativity,
for example, an infinite number of ways to solve the equations exist, and the
goal is to find solutions that match our universe. The overly ambitious string
theorists (the ones who expected a single vacuum to fall out of the sky) soon
realized that they, too, would end up with a rich string theory landscape,
as Leonard Susskind calls the range of possible vacua (see Chapter 11 for
more on the Susskind's landscape idea). The goal of string theory has since
become to figure out which set of vacua applies to our universe.
Looking into String Theory's Future
At present, string theory faces two hurdles. The first is the theoretical
hurdle, which is whether a model can be formulated that describes our own
universe. The second hurdle is the experimental one, because even if string
theorists are successful in modeling our universe, they'll then have to figure
out how to make a distinct prediction from the theory that's testable in
some way.
Right now, string theory falls short on both counts, and it's unclear whether
it can ever be formulated in a way that will be uniquely testable. The critics
claim that growing disillusionment with string theory is rising among theoret-
ical physicists, while the supporters continue to talk about how string theory
is being used to resolve the major questions of the universe.
Only time will tell whether string theory is right or wrong, but regardless of
the answer, string theory has driven scientists for years to ask fundamental
questions about our universe and explore the answers to those questions in
new ways. Even an alternative theory would in part owe its success to the
hard work performed by string theorists.
11%) Part I: Introducing String Theory _
Theoretical complications: Can
We figure out string theory}
The current version of string theory is called M-theory, introduced in 1995,
which is a comprehensive theory that includes the five supersymmetric
string theories. M-Theory exists in 11 dimensions. There's just one problem.
No one knows what M-theory is.
Scientists are searching for a complete string theory, but they don't have one
yet. And, until they do, there's no way of knowing that they'll be successful.
Until string theorists have a complete theory that describes our own universe,
the theory could all be smoke and mirrors. Although some aspects of string
theory may be shown to be true, it may be that these are only approximations
of some more fundamental theory — or it may be that string theory is actually
that fundamental theory itself.
String theory, the driving force of 21st-century theoretical physics, could
prove to be nothing more than a mathematical illusion that provides some
approximate insights into science but isn't actually the theory that drives the
forces of nature.
It's unclear how long the search for a theory can last without some specific
breakthrough. There's a sense (among some) that the most brilliant physi-
cists on the planet have been spinning their wheels for decades, with only a
handful of significant insights, and even those discoveries don't seem to lead
anywhere specific.
The theoretical implications of string theory are addressed in Chapters 10
and 11, while the criticism of the theory rears its ugly head in Chapter 17.
Experimental complications:
Can We pro(/e string theory)
Even if a precise version of string theory (or M-theory) is formulated, the
question then moves from the theoretical to the experimental realm. Right
now, the energy levels that scientists can reach in experiments are prob-
ably way too small to realistically test string theory, although aspects of the
theory can be tested today.
Theory moves forward with directions from experiment, but the last input
that string theory had from experiment was the realization that it failed as
a theory describing the scattering of particles within particle accelerators.
_ Chapter 3: Accomplishments and Failures of String Theory (l /
The realm string theory claims to explain involves distances so tiny that it's
questionable whether scientists will ever achieve a technology able to probe
at that length, so it's possible that string theory is an inherently untestable
theory of nature. (Some versions of string theory do make predictions in test-
able ranges, however, and string theorists hope that these versions of string
theory may apply to our universe.)
You find out some ways to possibly test string theory in Chapter 12, although
these are only speculative because right now science doesn't even have a
theory that makes any unique predictions. The best physicists can hope for
are some hints, such as the discovery of extra dimensions of certain types,
new cosmological predictions about the formation of our universe, or the
missing supersymmetric particles, that would give some direction to the
theoretical search.
UQ Part I: Introducing String Theory _
Part II
The Physics Upon
Which String
Theory Is Built
The 5 th Wave
By Rich Tennant
1905 At a lwch cowter in ?e«,
■Rmstem iormulates his Special
THeorg °4 'Relisnivitg.
In this part .
String theory is an evolution of concepts that have
been around for at least 300 years. To understand the
theory and its implications, you have to first understand
certain fundamental concepts, such as how scientific
theories develop.
In this part, you see how science progresses, which
will be helpful as you encounter the various scientific
revolutions that have led to string theory. I introduce
physics concepts at the heart of string theory, ranging
from the smallest distance measurable to the entire
universe. These overviews allow you to follow the later
string theory topics. However, the chapters in this part
don't even come close to providing complete explanations
of the fundamental topics from classical physics, relativity,
quantum physics, particle physics, and cosmology.
For more detailed introductions to the physics concepts
addressed in Part II, I recommend Physics For Dummies,
Einstein For Dummies, Quantum Physics For Dummies, and
Astronomy For Dummies, 2nd edition, (all published by
Wiley) as excellent starting points.
Chapter 4
Putting String Theory in Context:
Understanding the Method
of Science
In This Chapter
Brushing up on scientific theories you know and love
So you say you want a scientific revolution
What scientists have unified, let no one put asunder
Breaking the same old rules to keep things interesting
String theory is at the cutting edge of science. It's a mathematical theory
of nature that, at present, makes few predictions that are testable. This
begs the question of what it takes for a theory to be scientific.
In this chapter, I look a bit more closely at the methods scientists use to
investigate nature's structure. I explore how scientists perform science and
some of the ways that their work is viewed. I certainly don't solve any of
these big, philosophical issues in this chapter, but my goal is to make it clear
that scientists have differing views about how the nature of science is sup-
posed to work. Although I could write pages and pages on the evolution of
scientific thought throughout the ages, I touch on these topics in just enough
detail to help you understand some of the arguments in favor of and against
string theory.
y2 Part ll: The Physics Upon Which String Theory Is Built
Exploring the Practice of Science
Before you can figure out whether string theory is scientific, you have to ask,
"What is science?"
Science is the methodical practice of trying to understand and predict the
consequences of natural phenomena. This is done through two distinct but
closely related means: theory and experiment.
Not all science is created equal. Some science is performed with diagrams
and mathematical equations. Other science is performed with costly experi-
mental apparatus. Still other forms of science, while also costly, involve
observing distant galaxies for clues to the mystery of the universe.
String theory has spent more than 30 years focusing on the theory side of the
scientific equation and, sadly, is lacking on the experimental side, as critics
never hesitate to point out. Ideally, the theories developed would eventually
be validated by experimental evidence. (See the later sections "The need for
experimental falsifiability" and "The foundation of theory is mathematics" for
more on the necessity of experimentation.)
The myth of the scientific method
When in school, I was taught that science followed nice, simple rules called
the scientific method. These rules are a classical model of scientific investiga-
tion based on principles of reductionism and inductive logic. In other words,
you take observations, break them down (the reductionism part), and use
them to create generalized laws (the inductive logic part). String theory's his-
tory certainly doesn't follow this nice classical model.
In school, the steps of the scientific method actually changed a bit depend-
ing on the textbook I had in a given year, though they generally had mostly
common elements. Frequently, they were delineated as a set of bullet points:
(<" Observe a phenomenon: Look at nature
v" Formulate a hypothesis: Ask a question (or propose an answer)
(-" Test the hypothesis: Perform an experiment
v* Analyze the data: Confirm or reject the hypothesis
_ Chapter 4: Putting String Theory in Context J?3
Breaking down nature with Bacon
The ideas of the scientific method are often
traced back to Sir Francis Bacon's 1620 book
Novum Organum. It proposed that reduction-
ism and inductive reasoning could be used to
arrive at fundamental truths about the causes
of natural events.
In the Baconian model, the scientist breaks
natural phenomena down into component parts
that are then compared to other components
based on common themes. These reduced cat-
egories are then analyzed using principles of
inductive reasoning.
Inductive reasoning is a logical system of anal-
ysis where you start with specific true state-
ments and work to create generalized laws,
which would apply to all situations, by finding
commonalities between the observed truths.
In a way, this scientific method is a myth. I earned a degree in physics, with
honors no less, without once being asked a question about the scientific
method in a physics course. (It did come up in my Philosophy of Science
course, which you can thank for much of this chapter.)
Turns out there's no single scientific method that all scientists follow.
Scientists don't look at a list and think, "Well, I've observed my phenomenon
for the day. Time to formulate my hypothesis." Instead, science is a dynamic
activity that involves a continuous, active analysis of the world. It's an inter-
play between the world we observe and the world we conceptualize. Science
is a translation between observations, experimental evidence, and the
hypotheses and theoretical frameworks that are built to explain and expand
on those observations.
Still, the basic ideas of the scientific method do tend to hold. They aren't so
much hard and fast rules, but they're guiding principles that can be com-
bined in different ways depending on what's being studied.
The need for experimental falsi f lability
Traditionally, the idea has been that an experiment can either confirm or refute
a theory. An experimental result yields positive evidence if it supports the
theory, while a result that contradicts the hypothesis is negative evidence.
In the 20th century, a notion arose that the key to a theory — the thing that
makes it scientific — is whether it can in some way be shown to be false. This
principle of falsifiability can be controversial when applied to string theory,
which theoretically explores energy levels that can't at present (or possibly
ylf Part II: The Physics Upon Which String Theory Is Built _
j*JABE*
ever) be directly explored experimentally. Some claim that because string
theory currently fails the test of falsifiability, it's somehow not "real science."
(Check out Chapter 17 for more on this idea.)
The focus on this falsifiability is traced back to philosopher Karl Popper's
1934 book The Logic of Scientific Discovery. He was opposed to the reduction-
ist and inductive methods that Francis Bacon had popularized three centu-
ries earlier. In a time that was characterized by the rise of modern physics, it
appeared that the old rules no longer applied.
Popper reasoned that the principles of physics arose not merely by viewing
little chunks of information, but by creating theories that were tested and
repeatedly failed to be proved false. Observation alone could not have led to
these insights, he claimed, if they'd never been put in positions to be proven
false. In the most extreme form, this emphasis on falsifiability states that sci-
entific theories don't tell you anything definite about the world, but are only
the best guesses about the future based on past experience.
For example, if I predict that the sun will rise every morning, I can test this by
looking out my window every morning for 50 days. If the sun is there every
day, I have not proved that the sun will be there on the 51st day. After I actu-
ally observe it on the 51st day, I'll know that my prediction worked out again,
but I haven't proved anything about the 52nd day, the 53rd, and so on.
No matter how good a scientific prediction is, if you can run a test that shows
that it's false, you have to throw out the idea (or, at least, modify your theory
to explain the new data). This led the 19th century biologist Thomas Henry
Huxley to define the great tragedy of science as "the slaying of a beautiful
hypothesis by an ugly fact."
To Popper, this was far from tragic, but was instead the brilliance of science.
The defining component of a scientific theory, the thing that separates it
from mere speculation, is that it makes a falsifiable claim.
Popper's claim is sometimes controversial, especially when being used by
one scientist (or philosopher) to discredit an entire field of science. Many
still believe that reduction and inductive reasoning can, in fact, lead to the
creation of meaningful theoretical frameworks that represent reality as it is,
even if there's no claim that is falsifiable.
String theory founder Leonard Susskind makes just this argument. He
believes not in falsification, but rather in confirmation — you can have direct
positive evidence for a theory, rather than just a lack of negative evidence
against it.
_ Chapter 4: Putting String Theory in Context J J
This viewpoint comes out of an online debate between Susskind and physi-
cist Lee Smolin (you can view the debate atwww.edge.org/3rd_culture/
smolin_susskind04/smolin_susskind.html). In the debate, Susskind
lists several examples of theories that have been denounced as unfalsifiable:
behaviorism in psychology along with quark models and inflationary theory
in physics.
The examples he provides are cases where scientists believe that certain
traits couldn't be examined and methods were later developed that allowed
them to be tested. There's a difference between being unable to falsify a
theory in practice and being unable to falsify it in principle.
It may seem as if this debate over confirmation and falsifiability is academic.
That's probably true, but some physicists see string theory as a battle over
the very meaning of physics. Many string theory critics believe that it's inher-
ently unfalsifiable, while string theorists believe a mechanism to test (and
falsify) the prediction of string theory will be found.
The foundation of theory is mathematics
In physics, complex mathematical models are built that represent the under-
lying physical laws that nature follows. These mathematical models are the
real theories of physics that physicists can then relate to meaningful events
in the real world through experiment and other means.
Science requires both experiment and theory to build explanations of what
happens in the world. To paraphrase Einstein, science without theory is
lame, while science without experiment is blind.
If physics is built on a foundation of experimental observation, then theoreti-
cal physics is the blueprint that explains how those observations fit together.
The insights of theory have to move beyond the details of specific observa-
tions and connect them in new ways. Ideally, these connections lead to other
predictions that are testable by experiment. String theory has not yet made
this significant leap from theory to experiment.
A large part of the work in theoretical physics is developing mathematical
models — frequently including simplifications that aren't necessarily
realistic — that can be used to predict the results of future experiments.
When physicists "observe" a particle, they're really looking at data that con-
tains a set of numbers that they have interpreted as having certain character-
istics. When they look into the heavens, they receive energy readings that fit
certain parameters and explanations. To a physicist, these aren't "just" num-
bers; they're clues to understanding the universe.
56
Part II: The Physics Upon Which String Theory Is Built _
High-energy physics (which includes string theory and other physics at high
energies) has an intense interplay between theoretical insights and experi-
mental observations. Research papers in this area fall into one of four
categories:
Iv Experiment
J-" Lattice (computer simulations)
j-" Phenomenology
\* Theory
Phenomenology is the study of phenomena (no one ever said physicists were
creative when it comes to naming conventions) and relating them within the
framework of an existing theory. In other words, scientists focus on taking
the existing theory and applying it to the existing facts or build models
describing anticipated facts that may be discovered soon. Then they make
predictions about what experimental observations should be obtained. (Of
course, phenomenology has a lot more to it, but this is the basics of what you
need to know to understand it in relation to string theory.) It's an intriguing
discipline, and one that has, in recent years, begun to focus on supersym-
metry and string theory. When I discuss how to possibly test string theory
in Chapter 12, it is largely the work of phenomenologists that tells scientists
what they're looking for.
Though scientific research can be conducted with these different methods,
there is certainly overlap. Phenomenologists can work on pure theory and
can also, of course, prepare a computer simulation. Also, in some ways, a
computer simulation can be viewed as a process that is both experimental
and theoretical. But what all of these approaches have in common is that the
scientific results are expressed in the language of science: mathematics.
The rule of simplicity
In science, one goal is to propose the fewest "entities" or rules needed to
explain how something works. In many ways, the history of science is seen as
a progression of simplifying the complex array of natural laws into fewer and
fewer fundamental laws.
Take Occam's razor, which is a principle developed in the 14th century by
Franciscan friar and logician William of Occam. His "law of parsimony" is
basically translated (from Latin) as "entities must not be multiplied beyond
necessity." (In other words, keep it simple.) Albert Einstein famously stated
a similar rule as "Make everything as simple as possible, but not simpler."
Though not a scientific law itself, Occam's razor tends to guide how scientists
formulate their theories.
_ Chapter 4: Putting String Theory in Context f} /
In some ways, string theory seems to violate Occam's razor. For example, in
order for string theory to work, it requires the addition of a lot of odd com-
ponents (extra dimensions, new particles, and other features mentioned in
Chapters 10 and 11) that scientists haven't actually observed yet. However, if
these components are indeed necessary, then string theory is in accord with
Occam's razor.
The role of objectivity in science
Some people believe that science is purely objective. And, of course, science
is objective in the sense that the principles of science can be applied in the
same way by anyone and get the same results. But the idea that scientists
are themselves inherently objective is a nice thought, but it's about as true
as the notion of pure objectivity in journalism. The debate over string theory
demonstrates that the discussion isn't always purely objective. At its core,
the debate is over different opinions about how to view science.
In truth, scientists make choices continually that are subjective, such as
which questions to pursue. For example, when string theory founder Leonard
Susskind met Nobel Prize winner Murray Gell-Mann, Gell-Mann laughed at
the very idea of vibrating strings. Two years later, Gell-Mann wanted to hear
more about it.
In other words, physicists are people. They have learned a difficult discipline,
but this doesn't make them infallible or immune to pride, passion, or any
other human foible. The motivation for their decisions may be financial, aes-
thetic, personal, or any other reason that influences human decisions.
The degree to which a scientist relies on theory versus experiment in guid-
ing his activities is another subjective choice. Einstein, for example, spoke of
the ways in which only the "free inventions of the mind" (pure physical prin-
ciples, conceived in the mind and aided by the precise application of math-
ematics) could be used to perceive the deeper truths of nature in ways that
pure experiment never could. Of course, had experiments never confirmed
his "free inventions," it's unlikely that I or anyone else would be citing him a
century later.
Understanding How Scientific
Change 1$ Viewed
The debates over string theory represent fundamental differences in how
to view science. As the first part of this chapter points out, many people
have proposed ideas about what the goals of science should be. But over
yS Part ll: The Physics Upon Which String Theory Is Built _
the years, science changes as new ideas are introduced, and it's in trying to
understand the nature of these changes where the meaning of science really
comes into question.
The methods in which scientists adapt old ideas and adopt new ones can
also be viewed in different ways, and string theory is all about adapting old
ideas and adopting new ones.
Old becomes new again:
Science as revolution
The interplay between experiment and theory is never so obvious as in those
realms where they fail to match up. At that point, unless the experiment con-
tained a flaw, scientists have no choice but to adapt the existing theory to fit
the new evidence. The old theory must transform into a new theory. The phi-
losopher of science Thomas Kuhn spoke of such transformations as scientific
revolutions.
In Kuhn's model (which not all scientists agree with), science progresses
along until it accumulates a number of experimental problems that make sci-
entists redefine the theories that science operates under. These overarching
theories are scientific paradigms, and the transition from one paradigm to a
new one is a period of upheaval in science. In this view, string theory would
be a new scientific paradigm, and physicists would be in the middle of the
scientific revolution where it gains dominance.
A scientific paradigm, as proposed by Kuhn in his 1962 The Structure of
Scientific Revolutions, is a period of business as usual for science. A theory
explains how nature works, and scientists work within this framework.
Kuhn views the Baconian scientific method — regular puzzle-solving
activities — as taking place within an existing scientific paradigm. The scien-
tist gains facts and uses the rules of the scientific paradigm to explain them.
The problem is that there always seems to be a handful of facts that the sci-
entific paradigm can't explain. A few pieces of data don't seem to fit. During
the periods of normal science, scientists do their best to explain this data, to
incorporate it into the existing framework, but they aren't overly concerned
about these occasional anomalies.
That's fine when there are only a few such problems, but when enough of
them pile up, it can pose serious problems for the prevailing theory.
.Chapter 4: Putting String Theory in Context Jy
As these abnormalities begin to accumulate, the activity of normal science
becomes disrupted and eventually reaches the point where a full scientific
revolution takes place. In a scientific revolution, the current scientific para-
digm is replaced by a new one that offers a different conceptual model of
how nature functions.
At some point, scientists can't just proceed with business as usual anymore,
and they're forced to look for new ways to interpret the data. Initially, scien-
tists attempt to do this with minor modifications to the existing theory. They
can tack on an exception here or a special case there. But if there are enough
anomalies, and if these makeshift fixes don't resolve all the problems, scien-
tists are forced to build a new theoretical framework.
In other words, they are forced not only to amend their theory, but to con-
struct an entirely new paradigm. It isn't just that some factual details were
wrong, but their most basic assumptions were wrong. In a period of scientific
revolution, scientists begin to question everything they thought they knew
about nature. For example, in Chapter 10 you see that string theorists have
been forced to question the number of dimensions in the universe.
Combining forces: Science as unification
Science can be seen as a progressive series of unifications between ideas
that were, at one point, seen as separate and distinct. For example, biochem-
istry came about by applying the study of chemistry to systems in biology.
Together with zoology, this yields genetics and neo-darwinism — the modern
theory of evolution by natural selection, the cornerstone of biology.
In this way, we know that all biological systems are fundamentally chemical
systems. And all chemical systems, in turn, come from combining different
atoms to form molecules that ultimately follow the assorted laws defined in
the Standard Model of particle physics.
Physics, because it studies the most fundamental aspects of nature, is the
science most interested in these principles of unification. String theory, if
successful, might unify all fundamental physical forces of the universe down
to one single equation.
Galileo and Newton unified the heavens and Earth in their work in astronomy,
defining the motion of heavenly bodies and firmly establishing that Earth fol-
lowed exactly the same rules as all other bodies in our solar system. Michael
Faraday and James Clerk Maxwell unified the concepts of electricity and mag-
netism into a single concept governed by uniform laws — electromagnetism. (If
you want more information on gravity or electromagnetism, you'll be attracted
to Chapter 5.)
()0 Part II: The Physics Upon Which String Theory Is Built _
Albert Einstein, with the help of his old teacher Hermann Minkowski, uni-
fied the notions of space and time as dimensions of space-time, through his
theory of special relativity. In the same year, as part of the same theory, he
unified the concepts of mass and energy as well. Years later, in his general
theory of relativity, he unified gravitational force and special relativity into
one theory.
Central to quantum physics is the notion that particles and waves aren't the
separate phenomena that they appear to be. Instead, particles and waves
can be seen as the same unified phenomenon, viewed differently in different
circumstances.
The unification continued in the Standard Model of particle physics, when
electromagnetism was ultimately unified with the strong and weak nuclear
forces into a single framework.
^jjjUBEfl This process of unification has been astoundingly successful, because nearly
' /'^ _ ^ s \ everything in nature can be traced back to the Standard Model — except for
||||| ) gravity. String theory, if successful, will be the ultimate unification theory,
finally bringing gravity into harmony with the other forces.
What happens When you
break it) Science as symmetry
A symmetry exists when you can take something, transform it in some way,
and nothing seems to change about the situation. The principle of symme-
try is crucial to the study of physics and has special implications for string
theory in particular. When a transformation to the system causes a change in
the situation, scientists say that it represents a broken symmetry.
This is obvious in geometry. Take a circle and draw a line through its center,
as in Figure 4-1. Now picture flipping the circle around that line. The resulting
image is identical to the original image when flipped about the line. This is
linear or reflection symmetry. If you were to spin the figure 180 degrees, you'd
end up with the same image again. This is rotational symmetry. The trapezoid,
on the other hand, has asymmetry (or lacks symmetry) because no rotation
or reflection of the shape will yield the original shape.
The most fundamental form of symmetry in physics is the idea of transla-
tional symmetry, which is where you take an object and move it from one
location in space to another. If I move from one location to another, the laws
of physics should be the same in both places. This principle is how scientists
use laws discovered on Earth to study the distant universe.
_ Chapter 4: Putting String Theory in Context
61
In physics, though, symmetry means way more than just taking an object and
flipping, spinning, or sliding it through space.
The most detailed studies of energy in the universe indicate that, no matter
which direction you look, space is basically the same in all directions. The
universe itself seems to have been symmetric from the very beginning.
The laws of physics don't change over time (at least according to most physi-
cists and certainly not on short timescales, like a human lifetime or the entire
age of the United States of America). If I perform an experiment today and per-
form the same experiment tomorrow, I'll get essentially the same result. The
laws of physics possess a basic symmetry with respect to time. Changing the
time of something doesn't change the behavior of the system, though I discuss
some potential exceptions in Chapter 16.
These and other symmetries are seen as central to the study of science, and
in fact, many physicists have stated that symmetry is the single most impor-
tant concept for physics to grasp.
The truth is that while physicists often speak of the elegance of symmetry
in the universe, the string theorist Leonard Susskind is quite right when he
points out that things get interesting when the symmetry breaks.
In fact, as I was preparing for this book, the 2008 Nobel Prize in Physics was
awarded to three physicists — Yoichiro Nambu, Makoto Kobayashi, and
Toshihide Maskawa — for work in broken symmetry performed decades ago.
Without broken symmetry, everything would be absolutely uniform every-
where. The very fact that we have a chemistry that allows us to exist is proof
that some aspects of symmetry don't hold up in the universe.
Many theoretical physicists believe that a symmetry exists between the four
fundamental forces (gravity, electromagnetism, weak nuclear force, strong
nuclear force), a symmetry that broke early in the universe's formation and
causes the differences we see today. String theory is the primary (if not
(?2 Part I': The Physics Upon Which String Theory Is Built _
the only) means of understanding that broken symmetry, if it does (or did)
indeed exist.
This broken symmetry may be closely linked to supersymmetry, which is
necessary for string theory to become viable. Supersymmetry has been inves-
tigated in many areas of theoretical physics, even though there's no direct
experimental evidence for it, because it ensures that the theory includes
many desirable properties.
Supersymmetry and the unification of forces are at the heart of the string
theory story. As you read more about string theory, it's up to you to deter-
mine whether the lack of experimental evidence condemns it from the start.
Chapter 5
What You Must Know about
Classical Physics
In This Chapter
Matter and energy: Each affects the other
Transferring energy through waves and vibrations
Newton's four revolutionary breakthroughs
Electricity and magnetism: One in the same
J\]° matter now complex modern physics concepts get, they have their
# W roots in basic classical concepts. To understand the revolutions lead-
ing up to string theory, you need to first understand these basic concepts.
You'll then be able to understand how string theory recovers and generalizes
them.
In this chapter, I present some physics concepts that you need to be familiar
with to understand string theory. First, I discuss three fundamental concepts in
physics: matter, energy, and how they interact. Next I explain waves and vibra-
tions, which are crucial to understanding stringy behavior. Gravity is also key,
so Sir Isaac Newton's key discoveries come next. Finally, I give a brief overview
of electromagnetic radiation, an important aspect of physics that leads directly
into the discovery of both relativity and quantum physics — the two theories
that together give birth to modern string theory!
This Crazy Little Thirty Called Physics
Physics is the study of matter and its interactions. Physics tries to under-
stand the behavior of physical systems from the most fundamental laws that
we can achieve. String theory could provide the most fundamental law and
explain all of the universe in a single mathematical equation and physical
theory.
()(} Part II: The Physics Upon Which String Theory Is Built _
One other key principle of physics is the idea that many of the laws that
work in one location also work in another location — a principle known as
symmetry (I cover this in more detail later in this section and also in Chapter
4). This connection between physics in different locations is just one sort of
symmetry, allowing physics concepts to be related to each other. Science
has progressed by taking diverse concepts and unifying them into cohesive
physical laws.
This is a very broad definition of physics, but then physics is the broadest
science. Because everything you see, hear, smell, touch, taste, or in any way
interact with is made of matter and interacts according to some sort of rules,
that means that physics is literally the study of anything that happens. In a
way, chemistry and all the other sciences are approximations of the funda-
mental laws of physics.
Even if string theory (or some other "theory of everything") were to be found,
there would still be need for other sciences. Trying to figure out every single
physical system from string theory would be as absurd as trying to study the
weather by analyzing every single atom in the atmosphere.
No lauqhinq matter: What We're made of
One of the traits of matter (the "stuff" that everything is made of) is that it
requires force to do something. (There are some exceptions to this, but as
a rule a force is any influence that produces a change, or prevents a change,
in a physical quantity.) Mass is the property that allows matter to resist a
change in motion (in other words, the ability to resist force). Another key
trait of matter is that it's conserved, meaning it can't be created or destroyed,
but can only change forms. (Einstein's relativity showed this wasn't entirely
true, as you see in Chapter 6.)
Without matter, the universe would be a pretty boring place. Matter is all
around you. The book you're reading, as you lean back comfortably in your
matter-laden chair, is made of matter. You yourself are made of matter. But
what, exactly, is this stuff called matter?
Early philosophers and scientists try to understand matter
The question of matter's meaning dates back to at least the Greeks and
Chinese philosophers, who wondered what made one thing different from
another. Greek and Chinese thinkers noticed similar trends, and each devised
a system for categorizing matter into five fundamental elements based on
these common traits.
In ancient China, the five elements were metal, wood, water, fire, and earth.
Eastern religion and philosophy used these elements and the different ways
they interact to explain not only the natural world but also the moral realm.
_ Chapter 5: What You Must Know about Classical Physics %) J
Among the Greek philosophers, Aristotle is the most popular to have dis-
cussed their version of the five elements: fire, earth, air, water, and aether.
Aether was supposedly an unearthly, spiritual substance that filled the uni-
verse. In this view of matter, the realm outside of Earth was composed of this
aether and didn't undergo change the way our world does.
On Earth, material objects were seen as combinations of the basic elements.
For example, mud was a combination of water and earth. A cloud was a com-
bination of air and water. Lava was a combination of earth and fire.
In the 17th century, scientists' understanding of matter started to change
as astronomers and physicists began to realize that the same laws govern
matter both on Earth and in space. The universe isn't composed of eternal,
unchanging, unearthly aether, but of hard balls of ordinary matter.
Newton's key insight into the study of matter was that it resisted change in
motion (I explain this in more detail in the later "Force, mass, and accelera-
tion: Putting objects into motion" section). The degree to which an object
resists this change in motion is its mass.
Scientists discover that mass can't be destroyed
Antoine-Laurent Lavoisier's work in the 18th century provided physics with
another great insight into matter. Lavoisier and his wife, Marie Anne, per-
formed extensive experiments that indicated that matter can't be destroyed;
it merely changes from one form to another. This principle is called the con-
servation of mass.
This isn't an obvious property. If you burn a log, when you look at the pile of
ash, it certainly looks like you have a lot less matter than you started with.
But, indeed, Lavoisier found that if you're extremely careful that you don't
misplace any of the pieces — including the pieces that normally float away
during the act of burning — you end up with as much mass at the end of the
burning as you started with.
Over and over again, Lavoisier showed this unexpected trait of matter to
be the case, so much so that we now take it for granted as a familiar part of
our universe. Water may boil from liquid into gas, but the particles of water
continue to exist and can, if care is taken, be reconstituted back into liquid.
Matter can change form, but can't be destroyed (at least not until nuclear
reactions, which weren't discovered until well after Lavoisier's time).
As the study of matter progresses through time, things grow stranger instead
of more familiar. In Chapter 8, 1 discuss the modern understanding of matter,
in which we are composed mostly of tiny particles that are linked together
with invisible forces across vast (from their scale) empty distances. In fact,
as string theory suggests, it's possible that even those tiny particles aren't
really there — at least not in the way we normally picture them.
66
Part II: The Physics Upon Which String Theory Is Built _
Add a tittle energy: Why stuff happens
The matter in our universe would never do anything interesting if it weren't
for the addition of energy. There would be no change from hot to cold or
from fast to slow. Energy too is conserved, as discovered through the 1800s
as the laws of thermodynamics were explored, but the story of energy's con-
servation is more elusive than that of matter. You can see matter, but track-
ing energy proves to be trickier.
Kinetic energy is the energy involved when an object is in motion. Potential
energy is the energy contained within an object, waiting to be turned into
kinetic energy. It turns out that the total energy — kinetic energy plus poten-
tial energy — is conserved any time a physical system undergoes a change.
String theory makes predictions about physical systems that contain a large
amount of energy, packed into a very small space. The energies needed for
string theory predictions are so large that it might never be possible to con-
struct a device able to generate that much energy and test the predictions.
The energy of motion: Kinetic energy
Kinetic energy is most obvious in the case of large objects, but it's true at
all size levels. (I mean large objects in comparison to particles, so a grain of
sand and the planet both would be considered large in this case.) Heat (or
thermal energy) is really just a bunch of atoms moving rapidly, representing
a form of kinetic energy. When water is heated, the particles accelerate until
they break free of the bonds with other water molecules and become a gas.
The motion of particles can cause energy to emit in different forms, such as
when a burning piece of coal glows white hot.
Sound is another form of kinetic energy. If two billiard balls collide, the par-
ticles in the air will be forced to move, resulting in a noise. All around us, par-
ticles in motion are responsible for what takes place in our universe.
Stored energy: Potential energy
Potential energy, on the other hand, is stored energy. Potential energy takes
a lot more forms than kinetic energy and can be a bit trickier to understand.
A spring, for example, has potential energy when it's stretched out or com-
pressed. When the spring is released, the potential energy transforms into
kinetic energy as the spring moves into its least energetic length.
Moving an object in a gravitational field changes the amount of poten-
tial energy stored in it. A penny held out from the top of the Empire State
Building has a great deal of potential energy due to gravity, which turns into
a great deal of kinetic energy when dropped (although not, as evidenced
on an episode of MythBusters, enough to kill an unsuspecting pedestrian on
impact).
_ Chapter 5: What You Must Know about Classical Physics %} /
This may sound a bit odd, talking about something having more or less
energy just because of where it is, but the environment is part of the physical
system described by the physics equations. These equations tell exactly how
much potential energy is stored in different physical systems, and they can
be used to determine outcomes when the potential energy gets released.
Symmetry: Why some tarts
Were made to be broken
A change in location or position that retains the properties of the system is
called a geometric symmetry (or sometimes translational symmetry). Another
form of symmetry is an internal symmetry, which is when something within
the system can be swapped for something else and the system (as a whole)
doesn't change. When a symmetrical situation at high energy collapses into
a lower energy ground state that is asymmetrical, it's called spontaneous sym-
metry breaking. An example would be when a roulette wheel spins and slows
into a "ground state." The ball ultimately settles into one slot in the wheel —
and the gambler either wins or loses.
String theory goes beyond the symmetries we observe to predict even more
symmetries that aren't observed in nature. It predicts a necessary sym-
metry that's not observed in nature, called supersymmetry. At the energies
we observe, supersymmetry is an example of a broken symmetry, though
physicists believe that in high-energy situations, the supersymmetry would
no longer be broken (which is what makes it so interesting to study). 1 cover
supersymmetry in Chapters 2 and 10.
Translational symmetry: Same system, different spot
If an object has translational symmetry, you can move it and it continues to
look the same (for a detailed explanation of this, flip to Chapter 4). Moving
objects in space doesn't change the physical properties of the system.
Now, didn't I just say in the last section that the potential energy due to grav-
ity changes depending on where an object is? Yes, I did. Moving an object's
location in space can have an impact on the physical system, but the laws of
physics themselves don't change (so far as we can tell). If the Empire State
Building, Earth, and the penny held over the edge (the entire "system" in this
example) were all shifted by the same amount in the same direction, there
would be no noticeable change to the system.
Internal symmetry: The system changes,
hut the outcome stays the same
In an internal symmetry, some property of the system can undergo a change
without changing the outcome of the result.
()$ Part II: The Physics Upon Which String Theory Is Built _
For example, changing every particle with its antiparticle — changing posi-
tive charges to negative and negative charges to positive — leaves the elec-
tromagnetic forces involved completely identical. This is a form of internal
symmetry, called charge conjugation symmetry. Most internal symmetries
aren't perfect symmetries, meaning that they behave somewhat differently in
some situations.
Spontaneous symmetry breaking: A gradual breakdown
Physicists believe that the laws of the universe used to be even more sym-
metric, but have gone through a process called spontaneous symmetry break-
ing, where the symmetry falls apart in the universe we observe.
If everything were perfectly symmetric, the universe would be a very boring
place. The slight differences in the universe — the broken symmetries — are
what make the natural world so interesting, but when physicists look at the
physical laws, they tend to find that the differences are fairly small in com-
parison to the similarities.
To understand spontaneous symmetry breaking, consider a pencil perfectly
balanced on its tip. The pencil is in a state of perfect balance, of equilibrium,
but it's unstable. Any tiny disturbance will cause it to fall over. However, no
law of physics says which way the pencil will fall. The situation is perfectly
symmetrical because all directions are equal.
As soon as the pencil starts to fall, however, definite laws of physics dictate
the direction it will continue to fall. The symmetrical situation spontaneously
(and, for all intents and purposes, randomly) begins to collapse into one defi-
nite, asymmetrical form. As the system collapses, the other options are no
longer available to the system.
The Standard Model of particle physics, as well as string theory (which
includes the Standard Model as a low-energy approximation), predicts that
some properties of the universe were once highly symmetrical but have under-
gone spontaneous symmetry breaking into the universe we observe now.
All Shook Up: WaVes and Vibrations
In string theory, the most fundamental objects are tiny strings of energy that
vibrate or oscillate in regular patterns. In physics, such systems are called
harmonic oscillators, and much work has been done to study them.
Though the strings of string theory are different, understanding the vibrations
of classical objects — like air, water, jump-ropes, springs — can help you
understand the behavior of these exotic little creatures when you encounter
them. These classical objects can carry what are called mechanical waves.
_ Chapter 5: What You Must Know about Classical Physics
69
Catching the WaVe
Waves (as we usually think of them) move through some sort of medium. If
you flick the end of a jump-rope or string, a wave moves along the rope or
string. Waves move through the water, or sound waves through the air, with
those materials acting as the medium for the wave motion.
In classical physics, waves transport energy, but not matter, from one region
to another. One set of water molecules transfers its energy to the nearby
water molecules, which means that the wave moves through the water, even
though the actual water molecules don't actually travel all the way from the
start of the wave to the end of the wave.
This is even more obvious if I were to take the end of a jump-rope and shake
it, causing a wave to travel along its length. Clearly, the molecules at my end
of the jump-rope aren't traveling along it. Each group of jump-rope molecules
is nudging the next group of jump-rope molecules, and the end result is the
wave motion along its length.
There are two types of mechanical waves, as shown in Figure 5-1:
IJ-" Transverse wave: A wave in which the displacement of the medium is
perpendicular to the direction of travel of the wave along the medium,
like the flicking of a jump-rope.
J-" Longitudinal wave: A wave that moves in the same direction in which
the wave travels, like a piston pushing on a cylinder of water.
Transverse wave
The highest point on a transverse wave (or the densest point in a longitudi-
nal wave) is called a crest. The lowest point on a transverse wave (or the least
dense point in a longitudinal wave) is called a trough.
The displacement from the resting point to the crest — in other words, how
high the wave gets — is called the amplitude. The distance from one crest to
(0 Part II: The Physics Upon Which String Theory Is Built _
another (or one trough to another) is called the wavelength. These values are
shown on the transverse wave in Figure 5-1. The wavelength is shown on the
longitudinal wave, as well, although the amplitude is hard to show on that
type of wave, so it isn't included.
Another useful thing to consider is the velocity (speed and direction) of the
wave. This can be determined by its wavelength and frequency, which is a
measure of how many times the wave passes a given point per second. If you
know the frequency and the wavelength, you can calculate the velocity. This,
in turn, allows you to calculate the energy contained within the wave.
Another trait of many waves is the principle of superposition, which states
that when two waves overlap, the total displacement is the sum of the indi-
vidual displacements, as shown in Figure 5-2. This property is also referred to
as wave interference.
Figure 5-2:
When two
waves
overlap, the
total dis-
placement
is the sum
of the two
individual
displace-
ments.
-Wave#1
-Wave #2
Addition of Wave #1 and Wave #2
Consider waves when two ships cross each other's path. The waves made by
the ships cause the water to become choppier, and as the waves add height
to each other, they cause massive swells.
Similarly, sometimes waves can cancel each other out. If the crest of wave 1
overlaps with the trough of wave 2, they cancel each other out at that point.
This sort of interference plays a key role in one of the quantum physics prob-
lems I discuss in Chapter 7 — the double slit experiment.
Getting some good Vibrations
String theory depicts strings of energy that vibrate, but the strings are so tiny
that you never perceive the vibrations directly, only their consequences. To
_ Chapter 5: What You Must Know about Classical Physics / /
understand these vibrations, you have to understand a classical type of wave
called a standing wave — a wave that doesn't appear to be moving.
In a standing wave, certain points, called nodes, don't appear to move at
all. Other points, called antinodes, have the maximum displacement. The
arrangement of nodes and antinodes determines the properties of various
types of standing waves.
The simplest example of a standing wave is one with a node on each end,
such as a string that's fixed in place on the ends and plucked. When there is a
node on each end and only one antinode in between them, the wave is said to
vibrate at the fundamental frequency.
Consider a jump-rope that is held at each end by a child. The ends of the
rope represent nodes because they don't move much. The center of the rope
is the antinode, where the displacement is the greatest and where another
child will attempt to jump in. This is vibration at the fundamental frequency,
as demonstrated in Figure 5-3a.
represents (c)
the fun-
damental
frequency.
/2 Part ■■: The Physics Upon Which String Theory Is Built _
If the children get ambitious, however, and begin putting more energy into
the wave motion of their jump-rope, a curious thing happens. Eventually, the
children will pump enough energy into the rope that instead of one large anti-
node, two smaller antinodes are created, and the center of the rope seems to
be at rest, as shown in Figure 5-3b. It's almost as if someone grabbed hold of
the middle of the rope and gingerly, but firmly, is holding it in place!
A second type of standing wave can be considered if instead of a child hold-
ing each end of the rope, one end is mounted on a ring around a pole. The
child holding one end begins the wave motion, but the end on the pole is
now unconstrained and moves up and down. Instead of having a node on
each end, one end is a node (held by the child) and the other is an antinode
(moving up and down on the pole).
A similar situation in music happens when using a pipe that's closed at one
end and open at the other, such as in an organ. A node forms at the closed
end of the pipe, but the open end of the pipe is always an antinode.
A third type of standing wave has an antinode at each end. This would repre-
sent either a pipe that's open on both ends or a rope that's free to move on
both ends.
The more energy that's pumped into the standing wave, the more nodes form
(see Figure 5-3c). The series of frequencies that cause new nodes to form are
called harmonics. (In music, harmonics are called overtones.) The waves that
correspond to harmonics are called normal modes, or vibrational modes.
Music works because of the manipulation and superposition of harmonic
overtones created by these normal modes of vibration. The first three normal
modes are shown in Figure 5-3, where a string is fixed on both ends.
In string theory, the vibrational modes of strings (and other objects) are simi-
lar to those that I'm talking about in this chapter. In fact, matter itself is seen
as the manifestation of standing waves on strings. Different vibrational modes
give rise to different particles! We perceive the particles from the lowest vibra-
tional modes, but with higher energies, we may be able to detect other, higher-
energy particles.
Nekton's Revolution:
Physics Was Bow
How
Many see Sir Isaac Newton's discoveries as the start of modern physics
(along with a bit of help from his predecessor, Galileo Galilei). Newton's dis-
coveries dominated two centuries of physics, until Albert Einstein took his
place at the apex of scientific greatness.
_ Chapter 5: What You Must Know about Classical Physics / y
Newton's accomplishments are diverse, but he's known largely for four cru-
cial discoveries that define the realm of physics even today:
IJ-" Three laws of motion
J-" Law of universal gravitation
v* Optics
v* Calculus
Each of these discoveries has elements that will prove important as you
attempt to understand the later discoveries of string theory.
force, mass, and acceleration:
Putting objects into motion
Newton formulated three laws of motion, which showed his understanding
of the real meaning of motion and how it relates to force. Under his laws of
motion, a force created a proportional acceleration on an object.
This understanding was a necessary foundation upon which his law of grav-
ity was built (see the next section). In fact, both were introduced in his 1686
book Philosophiae Naturalis Principia Mathematica, a title that translates into
Mathematical Principles of Natural Philosophy. This book has become known
by the shorter title Principia in physics circles.
The second law of motion says that the force required to accelerate an object
is the product of the mass and acceleration, expressed by the equation F =
ma, where F is the total force, m is the object's mass, and a is the accelera-
tion. To figure out the total acceleration on an object, you figure out the total
forces acting on it and then divide by the mass.
Strictly speaking, Newton said that force was equal to the change in momen-
tum of an object. In calculus, this is the derivative of momentum with respect
to time. Momentum is equal to mass times velocity. Because mass is assumed
to be constant and the derivative of velocity with respect to time yields the
acceleration, the popular F= ma equation is a simplified way of looking at this
situation.
This equation can also be used to define mass. If I take a force and divide it by
the acceleration it causes on an object, I can determine the mass of the object.
One question which string theorists hope to answer is why some objects have
mass and others (such as the photon) do not.
7 Q, Part II: The Physics Upon Which String Theory Is Built _
Newton makes some laws about motion
The second law, and the way it relates force,
acceleration, and mass, is the only law of
motion relevant to a string theory discussion.
However, for true Newton-o-philes, here are
the other two laws of motion, paraphrased for
ease of understanding:
v* Newton's first law of motion: An object at
rest remains at rest, or an object in motion
remains in motion, unless acted upon by
an external force. In other words, it takes a
force to cause motion to change.
U* Newton's third law of motion: When two
objects interact through a force, each
object exerts a force on the other object
that is equal and opposite. In other words,
if I exert a force on the wall with my hand,
the wall exerts an equal force back on my
hand.
Gravity: A great discovery
With the laws of motion in hand, Newton was able to perform the action that
would make him the greatest physicist of his age: explaining the motion of
the heavens and the Earth. His proposal was the law of universal gravitation,
which defines a force acting between two objects based on their masses and
the distance separating them.
The more massive the objects, the higher the gravitational force is. The rela-
tionship with distance is an inverse relationship, meaning that as the distance
increases, the force drops off. (It actually drops off with the square of the
distance — so it drops off very quickly as objects are separated.) The closer
two objects are, the higher the gravitational force is.
The strength of the gravitational force determines a value in Newton's equa-
tion, called the gravitational constant or Newton's constant. This value is
obtained by performing experiments and observations, and calculating what
the constant should be. One question still open to physics and string theory
is why gravity is so weak compared to other forces.
Gravity seems fairly straightforward, but it actually causes quite a few prob-
lems for physicists, because it won't behave itself and get along with the other
forces of the universe. Newton himself wasn't comfortable with the idea of a
force acting at a distance, without understanding the mechanism involved.
But the equations, even without a thorough explanation for what caused it,
worked. In fact, the equations worked well enough that for more than two
centuries, until Einstein, no one could figure out what was missing from the
theory. More on this in Chapter 6.
Chapter 5: What You Must Know about Classical Physics / f}
Optics: Shedding light on light's properties
Newton also performed extensive work in understanding the properties of
light, a field known as optics. Newton supported a view that light moved as
tiny particles, as opposed to a theory that light traveled as a wave. Newton
performed all of his work in optics assuming that light moved as tiny balls of
energy flying through the air.
For nearly a century, Newton's view of light as particles dominated, until
Thomas Young's experiments in the early 1800s demonstrated that light
exhibited the properties of waves, namely the principle of superposition (see
the earlier "Catching the wave" section for more on superposition and the
later "Light as a wave: The ether theory" section for more on light waves).
The understanding of light, which began with Newton, would lead to the
revolutions in physics by Albert Einstein and, ultimately, to the ideas at the
heart of string theory. In string theory, both gravity and light are caused by
the behavior of strings.
Calculus and mathematics: Enhancing
scientific understanding
To study the physical world, Newton had to develop new mathematical
tools. One of the tools he developed was a type of math that we call calculus.
Actually, at the same time he invented it, philosopher and mathematician
Gottfried Leibniz had also created calculus completely independently! Newton
needed calculus to perform his analysis of the natural world. Leibniz, on the
other hand, developed it mainly to explain certain geometric problems.
Think for a moment how amazing this really is. A purely mathematical con-
struct, like calculus, provided key insights into the physical systems that
Newton explored. Alternately, the physical analysis that Newton performed
led him to create calculus. In other words, this is a case where mathematics
and science seemed to help build upon each other! One of the major suc-
cesses of string theory is that it has provided motivation for important math-
ematical developments that have gone on to be useful in other realms.
The Forces of Light: Electricity
and Magnetism
In the 19th century, the physical understanding of the nature of light changed
completely. Experiments began to show strong cases where light acted like
76
Part II: The Physics Upon Which String Theory Is Built _
waves instead of particles, which contradicted Newton (see the "Optics:
Shedding light on light's properties" section for more on Newton's findings).
During the same time, experiments into electricity and magnetism began to
reveal that these forces behaved like light, except that we couldn't see them!
By the end of the 19th century, it became clear that electricity and magne-
tism were different manifestations of the same force: electromagnetism. One
of the goals of string theory is to develop a single theory that incorporates
both electromagnetism and gravity.
Light as a WaOe: The ether theory
Newton had treated light as particles, but experiments in the 19th century
began to show that light acted like a wave. The major problem with this was
that waves require a medium. Something has to do the waving. Light seemed
to travel through empty space, which contained no substance at all. What
was the medium that light used to move through? What was waving?
To explain the problem, physicists proposed that space was filled with a sub-
stance. When looking for a name for this hypothetical substance, physicists
turned back to Aristotle and named it luminous ether. (Some physicists con-
tinued to spell it aether, but I call it ether to distinguish it from Aristotle's fifth
element.)
Even with this hypothetical ether, though, there were still problems.
Newton's optics still worked, and his theory described light in terms of tiny
balls moving in straight lines, not as waves! It seemed that sometimes light
acted like a wave and sometimes it acted as a particle.
Most physicists of the 19th century believed in the wave theory, largely
because the study of electricity and magnetism helped support the idea that
light was a wave, but they were unable to find solid evidence of the ether.
Invisible lines of force: Electric
and magnetic fields
Electricity is the study of how charged particles affect each other. Magnetism,
on the other hand, is the study of how magnetized objects affect each other.
In the 19th century, research began to show that these two seemingly sepa-
rate phenomena were, in fact, different aspects of the same thing. The physi-
cist Michael Faraday proposed that invisible fields transmitted the force.
_ Chapter 5: What You Must Know about Classical Physics / /
Electricity and magnetism are (inked together
An electrical force acts between two objects that contain a property called
electrical charge that can be either positive or negative. Positive charges
repel other positive charges, and negative charges repel other negative
charges, but positive and negative charges attract each other, as in Figure 5-4.
Coulomb's Law, which describes the simplest behavior of the electric force
between charged particles (a field called electrostatics), is an inverse square
law, similar to Newton's law of gravity. This provided some of the first
inklings that gravity and electrostatic forces (and, ultimately, electromagne-
tism) might have something in common.
Like repels
like, but
© 0^>
When electrical charges move, they create an electrical current. These cur-
rents can influence each other through a magnetic force. This was discovered
by Hans Christian Oersted, who found that a wire with an electrical current
running through it could deflect the needle of a compass.
Later work by Michael Faraday and others showed that this worked the other
way, as well — a magnetic force can influence an electrical current. As dem-
onstrated in Figure 5-5, moving a magnet toward a conducting loop of wire
causes a current to run through the wire.
Figure 5-5:
A magnet
moving
toward a
metal ring
creates a
current in
the ring.
r^^^-
/$ Part II: The Physics Upon Which String Theory Is Built _
Faraday proposes force fields to explain these forces
In the 1840s, Michael Faraday proposed the idea that invisible lines of force
were at work in electrical currents and magnetism. These hypothetical lines
made up a force field that had a certain value and direction at any given point
and could be used to calculate the total force acting on a particle at that
point. This concept was quickly adapted to also apply to gravity in the form
of a gravitational field.
These invisible lines of force were responsible for the electrical force (as
shown in Figure 5-6) and magnetic force (as shown in Figure 5-7). They
resulted in an electric field and a magnetic field that could be measured.
Figure 5-7:
The north
and south
poles of a
bar magnet
are con-
nected
by invis-
ible lines of
force.
Faraday proposed the invisible lines of force, but wasn't nearly as clear on
how the force was transmitted, which drew ridicule from his peers. Keep in
mind, though, that Newton also couldn't fully explain how gravity was trans-
mitted, so there was precedent to this. Action at a distance was already an
established part of physics, and Faraday, at least, was proposing a physical
model of how it could take place.
_ Chapter 5: What You Must Know about Classical Physics fy
The fields proposed by Faraday turned out to have applications beyond
electricity and magnetism. Gravity, too, could be written in a field form. The
benefit of a force field is that every point in space has a value and direction
associated with it. If you can calculate the value of the field at a point, you
know exactly how the force will act on an object placed at that point. Today,
every law of physics can be written in the form of fields.
Maxwell's equations briny it all together:
Electromagnetic Waties
Physicists now know that electricity and magnetism are both aspects of the
same electromagnetic force. This force travels in the form of electromagnetic
waves. We see a certain range of this electromagnetic energy in the form of
visible light, but there are other forms, such as X-rays and microwaves, that
we don't see.
In the mid-1800s, James Clerk Maxwell took the work of Faraday and others
and created a set of equations, known as Maxwell's equations, that described
the forces of electricity and magnetism in term of electromagnetic waves. An
electromagnetic wave is shown in Figure 5-8.
Maxwell's equations allowed him to calculate the exact speed that the elec-
tromagnetic wave traveled. When Maxwell performed this calculation, he was
amazed to find that he recognized the value. Electromagnetic waves moved
at exactly the speed of light!
Maxwell's equations showed that visible light and electromagnetic waves are
different manifestations of the same underlying phenomena. In other words,
we see only a small range of the entire spectrum of electromagnetic waves
that exist in our universe. Extending this unification to include all the forces of
nature, including gravity, would ultimately lead to theories of quantum gravity
such as string theory.
Q Q Part II: The Physics Upon Which String Theory Is Built
Two dark clouds and the
birth of modern physics
Two significant unanswered questions with the electromagnetic theory
remained. The first problem was that the ether hadn't been detected, while
the second involved an obscure problem about energy radiation, called the
blackbody problem (described in Chapter 7). What's amazing, in retrospect,
is that physicists didn't see these problems (or dark clouds as British scien-
tist Lord Kelvin called them in a 1900 speech) as especially significant, but
instead believed that they were minor issues that would soon be resolved. As
you see in Chapters 6 and 7, resolving these two problems would introduce
the great revolutions of modern physics — relativity and quantum physics.
Chapter 6
Revolutionizing Space and Time:
Einstein's Relativity
In This Chapter
Looking for something that allows light waves to travel
Nailing down the relationships between space and time, and mass and energy
Grasping the forces behind gravity
Meeting one of string theory's forerunners
/M lbert Einstein introduced his theory of relativity to explain the issues
v \ arising from the electromagnetic concepts introduced in Chapter 5.
The theory has had far-reaching implications, altering our understanding of
time and space. It provides a theoretical framework that tells us how grav-
ity works, but it has left open certain questions that string theory hopes to
answer.
In this book, I give you only a glimpse of relativity — the glimpse needed to
understand string theory. For a more in-depth look at the fascinating con-
cepts of Einstein's theory of relativity, I suggest Einstein For Dummies by
Carlos I. Calle, PhD (Wiley).
In this chapter, I explain how the ether model failed to match experimental
results and how Einstein introduced special relativity to resolve the problem.
I discuss Einstein's theory of gravity in general relativity, including a brief
look at a rival theory of gravity and how Einstein's theory was confirmed.
I then point out some issues arising from relativity. Finally, I introduce a
theory that tried to unify relativity and electromagnetics and is seen by many
as a predecessor of string theory.
$2 Part I': The Physics Upon Which String Theory Is Built _
What Waves Light Wai/es>
Searching (or the Ether
In the latter part of the 19th century, physicists were searching for the mys-
terious ether — the medium they believed existed for light waves to wave
through. Their inability to discover this ether, despite good experiments, was
frustrating, to say the least. Their failure paved the way for Einstein's expla-
nation, in the form of the theory of relativity.
As I explain in Chapter 5, waves had to pass through a medium, a substance
that actually did the waving. Light waves pass through "empty space" of a
vacuum (a space without any air or other regular matter), so physicists had
predicted a luminous ether that must exist everywhere and be some sort of
substance that scientists had never before encountered. In other words, the
"empty space" was not (in the view of the time) really empty because it con-
tained ether.
Some things could be predicted about the ether, though. For example, if
there was a medium for light, the light was moving through it, like a swim-
mer moving through the water. And, like a swimmer, the light should travel
slightly faster when going in the same direction as the water's current than
when the swimmer is trying to go against the water's current.
This doesn't mean that the ether itself was moving. Even if the ether was com-
pletely still, Earth was moving within the ether, which is effectively the same
thing. If you walk through a still body of water, it feels basically the same as if
you were walking in place and the water was flowing around you. (In fact, they
now have small pools that use this exact principle. You can swim for hours
in a pool that's only a few feet long. Because a powerful current is pumping
through it, you swim against the current and never go anywhere.)
Physicists wanted to construct an experiment based on this concept that
would test whether light traveled different speeds in different directions.
This sort of variation would support the idea that light was traveling through
an ether medium.
In 1881, physicist Albert Michelson created a device called an interferometer
designed to do just that. With the help of his colleague Edward Morley, he
improved the design and precision of the device in 1887. The Michelson-
Morley interferometer is shown in Figure 6-1.
_ Chapter 6: Revolutionizing Space and Time: Einstein's Relativity Oj
Figure 6-1:
The
Michelson-
Morley
interferom-
eter sends
light beams
along two
different
paths to
meet up on
a screen.
41
ii Screen
The interferometer used mirrors that were only partially reflective, so they
let half the light pass through and reflected half the light. The interferometer
set these mirrors at an angle, splitting a single beam of light so it ended up
traveling two different paths. The paths traveled perpendicular to each other,
but ended up hitting the same screen.
In 1887, Michelson and Morley ran a series of tests with the improved inter-
ferometer to discover the ether. They thought that the light traveling along
one of these paths should be slightly faster than the light traveling along the
other path, because one of them would be going either with or against the
ether, and the other path would be perpendicular to the ether. When the
light hit the screen, each beam would have traveled the exact same distance.
If one had traveled a slightly different speed, the two beams would be slightly
out of phase with each other, which would show distinctive wave interfer-
ence patterns — light and dark bands would appear — on the screen.
No matter how many times Michelson and Morley conducted the experi-
ment, they never found this difference in speed for the two light beams. They
always found the same speed of approximately 670 million miles per hour,
regardless of the direction the light traveled.
Physicists didn't immediately dismiss the ether model; instead they (includ-
ing Michelson and Morley) considered it a failed experiment, even though it
should have worked had there been an ether. In 1900, when Lord Kelvin gave
his "two dark clouds" speech, 13 years had passed without being able to
detect the ether's motion, but it was still assumed that the ether existed.
Sometimes scientists are reluctant to give up on a theory that they've devoted
years to, even if the evidence turns against them — something that the critics
|Mj| J of string theory believe may be happening right now in the theoretical physics
community.
$ [} Part II: The Physics Upon Which String Theory Is Built
No Ether7 No Problem: Introducing
Special Relativity
In 1905, Albert Einstein published a paper explaining how to have electro-
magnetics work without an ether. This theory came to be known as the theory
of special relativity, which explains how to interpret motion between differ-
ent inertial frames of reference — that is, places that are moving at constant
speeds relative to each other.
The key to special relativity was that Einstein explained the laws of phys-
ics when two objects are moving at a constant speed as the relative motion
between the two objects, instead of appealing to the ether as an absolute
frame of reference that defined what was going on. If you and some astro-
naut, Amber, are moving in different spaceships and want to compare your
observations, all that matters is how fast you and Amber are moving with
respect to each other.
Special relativity includes only the special case (hence the name) where
the motion is uniform. The motion it explains is only if you're traveling in a
straight line at a constant speed. As soon as you accelerate or curve — or do
anything that changes the nature of the motion in any way — special relativ-
ity ceases to apply. That's where Einstein's general theory of relativity comes
in, because it can explain the general case of any sort of motion. (I cover this
theory later in the chapter.)
Einstein's 1905 paper that introduced special relativity, "On the
Electrodynamics of Moving Bodies," was based on two key principles:
V The principle of relativity: The laws of physics don't change, even for
objects moving in inertial (constant speed) frames of reference.
J-" The principle of the speed of light: The speed of light is the same for
all observers, regardless of their motion relative to the light source.
(Physicists write this speed using the symbol c.)
The genius of Einstein's discoveries is that he looked at the experiments and
assumed the findings were true. This was the exact opposite of what other
physicists seemed to be doing. Instead of assuming the theory was correct
and that the experiments failed, he assumed that the experiments were cor-
rect and the theory had failed.
The ether had caused a mess of things, in Einstein's view, by introducing a
medium that caused certain laws of physics to work differently depending
on how the observer moved relative to the ether. Einstein just removed the
ether entirely and assumed that the laws of physics, including the speed of
light equal to c, worked the same way regardless of how you were moving —
exactly as experiments and mathematics showed them to be!
_ Chapter 6: Revolutionizing Space and Time: Einstein's Relativity Oj
Giving credit where credit is due
No physicist works in a vacuum, and that was
certainly true of Albert Einstein. Though he rev-
olutionized the world of physics, he did so by
resolving the biggest issues of his day, which
means he was tackling problems that a lot of
other physicists were also working on. He had
a lot of useful research to borrow from. Some
have accused Einstein of plagiarism, or implied
that his work wasn't truly revolutionary because
he borrowed so heavily from the work of others.
For example, his work in special relativity was
largely based on the work of Hendrik Lorentz,
George FitzGerald, and Jules Henri Poincare,
who had developed mathematical transforma-
tions that Einstein would later use in his theory
of relativity. Essentially, they did the heavy lift-
ing of creating special relativity, but they fell
short in one important way — they thought it
was a mathematical trick, not a true represen-
tation of physical reality.
The same is true of the discovery of the photon.
Max Planck introduced the idea of energy
in discrete packets, but thought it was only a
mathematical trick to resolve a specific odd
situation. Einstein tookthe mathematical results
literally and created the theory of the photon.
The accusations of plagiarism are largely dis-
missed by the scientific community because
Einstein never denied that the work was done
by others and, in fact, gave them credit when he
was aware of their work. Physicists tend to rec-
ognize the revolutionary nature of Einstein's work
and know that others contributed greatlyto it.
Unifying space and time
Einstein's theory of special relativity created a fundamental link between space
and time. The universe can be viewed as having three space dimensions —
up/down, left/right, forward/backward — and one time dimension. This
4-dimensional space is referred to as the space-time continuum.
If you move fast enough through space, the observations that you make
about space and time differ somewhat from the observations that other
people, who are moving at different speeds, make. The formulas Einstein
used to describe these changes were developed by Hendrik Lorentz (see the
nearby sidebar, "Giving credit where credit is due").
String theory introduces many more space dimensions, so grasping how the
dimensions in relativity work is a crucial starting point to understanding some
of the confusing aspects of string theory. The extra dimensions are so impor-
tant to string theory that they get their own chapter, Chapter 13.
Following the bouncing beam of tight
The reason for this space-time link comes from applying the principles of
relativity and the speed of light very carefully. The speed of light is the dis-
tance light travels divided by the time it takes to travel this path, and (accord-
ing to Einstein's second principle) all observers must agree on this speed.
86
Part II: The Physics Upon Which String Theory Is Built _
Sometimes, though, different observers disagree on the distance a light beam
has traveled, depending on how they're moving through space.
This means that to get the same speed those observers must disagree about
the time the light beam travels the given distance.
You can picture this for yourself by understanding the thought experiment
depicted in Figure 6-2. Imagine that you're on a spaceship and holding a laser
so it shoots a beam of light directly up, striking a mirror you've placed on the
ceiling. The light beam then comes back down and strikes a detector.
However, the spaceship is traveling at a constant speed of half the speed of
light (0.5c, as physicists would write it). According to Einstein, this makes no
difference to you — you can't even tell that you're moving. However, if astro-
naut Amber were spying on you, as in the bottom of Figure 6-2, it would be a
different story.
Amber would see your beam of light travel upward along a diagonal path,
strike the mirror, and then travel downward along a diagonal path before
striking the detector. In other words, you and Amber would see different
paths for the light and, more importantly, those paths aren't even the same
length. This means that the time the beam takes to go from the laser to the
mirror to the detector must also be different for you and Amber so that you
both agree on the speed of light.
_ Chapter 6: Revolutionizing Space and Time: Einstein's Relativity q /
This phenomenon is known as time dilation, where the time on a ship moving
very quickly appears to pass slower than on Earth. In Chapter 16, 1 explain
some ways that this aspect of relativity can be used to allow time travel. In
fact, it allows the only form of time travel that scientists know for sure is
physically possible.
As strange as it seems, this example (and many others) demonstrates that in
Einstein's theory of relativity, space and time are intimately linked together.
If you apply Lorentz transformation equations, they work out so that the
speed of light is perfectly consistent for both observers.
jMSE/? This strange behavior of space and time is only evident when you're traveling
close to the speed of light, so no one had ever observed it before. Experiments
lM|| ) carried out since Einstein's discovery have confirmed that it's true — time and
space are perceived differently, in precisely the way Einstein described, for
objects moving near the speed of light.
Building the space-time continuum
Einstein's work had shown the connection between space and time. In
fact, his theory of special relativity allows the universe to be shown as a
4-dimensional model — three space dimensions and one time dimension. In
this model, any object's path through the universe can be described by its
worldline through the four dimensions.
Though the concept of space-time is inherent in Einstein's work, it was
actually an old professor of his, Hermann Minkowski, who developed the
concept into a full, elegant mathematical model of space-time coordinates in
1907. Actually, Minkowski had been specifically unimpressed with Einstein,
famously calling him a "lazy dog."
One of the elements of this work is the Minkowski diagram, which shows the
path of an object through space-time. It shows an object on a graph, where
one axis is space (all three dimensions are treated as one dimension for sim-
plicity) and the other axis is time. As an object moves through the universe,
its sequence of positions represents a line or curve on the graph, depend-
ing on how it travels. This path is called the object's worldline, as shown
in Figure 6-3. In string theory, the idea of a worldline becomes expanded to
include the motion of strings, into objects called worldsheets. (See Chapter 16
for more information. A worldsheet can be seen in Figure 16-1.)
Unifying mass and energy
The most famous work of Einstein's life also dates from 1905 (a very busy
year for him), when he applied the ideas of his relativity paper to come up
with the equation E=mc 2 that represents the relationship between mass (m)
and energy (E).
S8 Part ll: The Physics Upon Which String Theory Is Built _
Figure 6-3:
The path
a par-
ticle takes
through
space
and time
creates its
worldline.
The reason for this connection is a bit involved, but essentially it relates to
the concept of kinetic energy discussed in Chapter 5. Einstein found that as
an object approached the speed of light, c, the mass of the object increased.
The object goes faster, but it also gets heavier. In fact, if it were actually able
to move at c, the object's mass and energy would both be infinite. A heavier
object is harder to speed up, so it's impossible to ever actually get the par-
ticle up to a speed of c.
In this 1905 paper — "Does the Inertia of a Body Depend on its Energy
Content?" — Einstein showed this work and extended it to stationary matter,
showing that mass at rest contains an amount of energy equal to mass
times c 2 .
Until Einstein, the concepts of mass and energy were viewed as completely
separate. He proved that the principles of conservation of mass and conserva-
tion of energy are part of the same larger, unified principle, conservation of
mass-energy. Matter can be turned into energy and energy can be turned into
matter because a fundamental connection exists between the two types of
substance.
If you're interested in greater detail on the relationship of mass and energy,
check out Einstein For Dummies (Wiley) or the book E=mc 2 : A Biography of the
World's Most Famous Equation by David Bodanis (Walker & Company).
Chapter 6: Revolutionizing Space and Time: Einstein's Relativity Oy
Changing Course: Introducing
General Relativity
General relativity was Einstein's theory of gravity, published in 1915,
which extended special relativity to take into account non-inertial frames of
reference — areas that are accelerating with respect to each other. General
relativity takes the form of field equations, describing the curvature of space-
time and the distribution of matter throughout space-time. The effects of
matter and space-time on each other are what we perceive as gravity.
Gravity as acceleration
Einstein immediately realized that his theory of special relativity worked
only when an object moved in a straight line at a constant speed. What about
when one of the spaceships accelerated or traveled in a curve?
Einstein came to realize the principle that would prove crucial to developing
his general theory of relativity. He called it the principle of equivalence, and
it states that an accelerated system is completely physically equivalent to a
system inside a gravitational field.
As Einstein later related the discovery, he was sitting in a chair thinking
about the problem when he realized that if someone fell from the roof of a
house, he wouldn't feel his own weight. This suddenly gave him an under-
standing of the equivalence principle.
As with most of Einstein's major insights, he introduced the idea as a thought
experiment. If a group of scientists were in an accelerating spaceship and
performed a series of experiments, they would get exactly the same results
as if sitting still on a planet whose gravity provided that same acceleration,
as shown in Figure 6-4.
Einstein's brilliance was that after he realized an idea applied to reality, he
applied it uniformly to every physics situation he could think of.
For example, if a beam of light entered an accelerating spaceship, then the
beam would appear to curve slightly, as in the left picture of Figure 6-5. The
beam is trying to go straight, but the ship is accelerating, so the path, as
viewed inside the ship, would be a curve.
By the principle of equivalence, this meant that gravity should also bend
light, as shown in the right picture of Figure 6-5. When Einstein first realized
this in 1907, he had no way to calculate the effect, other than to predict that
it would probably be very small. Ultimately, though, this exact effect would
be the one used to give general relativity its strongest support.
y Q Part II: The Physics Upon Which String Theory Is Built _
Figure 6-5:
Both accel-
eration and
gravity bend
a beam of
light.
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_ Chapter 6: Revolutionizing Space and Time: Einstein's Relativity y /
Gravity as geometry
The theory of the space-time continuum already existed, but under general
relativity Einstein was able to describe gravity as the bending of space-time
geometry. Einstein defined a set of field equations, which represented the way
that gravity behaved in response to matter in space-time. These field equa-
tions could be used to represent the geometry of space-time that was at the
heart of the theory of general relativity.
As Einstein developed his general theory of relativity, he had to refine
Minkowski's notion of the space-time continuum into a more precise math-
ematical framework (see the earlier "Building the space-time continuum"
section for more on this concept). He also introduced another principle, the
principle of covariance. This principle states that the laws of physics must
take the same form in all coordinate systems.
In other words, all space-time coordinates are treated the same by the laws
of physics — in the form of Einstein's field equations. This is similar to the
relativity principle, which states that the laws of physics are the same for
all observers moving at constant speeds. In fact, after general relativity was
developed, it was clear that the principles of special relativity were a special
case.
Einstein's basic principle was that no matter where you are — Toledo, Mount
Everest, Jupiter, or the Andromeda galaxy — the same laws apply. This time,
though, the laws were the field equations, and your motion could very defi-
nitely impact what solutions came out of the field equations.
Applying the principle of covariance meant that the space-time coordinates
in a gravitational field had to work exactly the same way as the space-time
coordinates on a spaceship that was accelerating. If you're accelerating
through empty space (where the space-time field is flat, as in the left picture
of Figure 6-6), the geometry of space-time would appear to curve. This meant
that if there's an object with mass generating a gravitational field, it had to
curve the space-time field as well (as shown in the right picture of Figure 6-6).
Figure 6-6:
Without
matter,
space-time
is flat (left),
but it curves
when matter
is present
(right).
y 2 Part I': The Physics Upon Which String Theory Is Built
/ #\ In other words, Einstein had succeeded in explaining the Newtonian mystery
IHJJ ) of where gravity came from! Gravity resulted from massive objects bending
space-time geometry itself.
Because space-time curved, the objects moving through space would follow
the "straightest" path along the curve, which explains the motion of the plan-
ets. They follow a curved path around the sun because the sun bends space-
time around it.
Again, you can think of this by analogy. If you're flying by plane on Earth, you
follow a path that curves around the Earth. In fact, if you take a flat map and
draw a straight line between the start and end points of a trip, that would not
be the shortest path to follow. The shortest path is actually the one formed
by a "great circle" that you'd get if you cut the Earth directly in half, with both
points along the outside of the cut. Traveling from New York City to northern
Australia involves flying up along southern Canada and Alaska — nowhere
close to a straight line on the flat maps we're used to.
Similarly, the planets in the solar system follow the shortest paths — those
that require the least amount of energy — and that results in the motion we
observe.
Testing general retatioity
For most purposes, the theory of general relativity matched the predictions
of Newton's gravity, and it also incorporated special relativity — it was a rela-
tivists theory of gravity. But no matter how impressive a theory is, it still has
to be confirmed by experiment before the physics community fully embraces
it. Today, scientists have seen extensive evidence of general relativity.
One stunning modern example of applying relativity is the global positioning
system (GPS). The GPS satellite system sends carefully synchronized beams
around the planet. This is what allows military and commercial devices to
know their location to within a few meters or better. But the entire system
is based upon the synchronization of these satellites that had to be pro-
grammed with corrections to take into account the curvature of space-time
near Earth. Without these corrections, minor timing errors would accumulate
day after day, causing the system to completely break down.
Of course, such equipment wasn't available to Einstein when he published
his theory in 1915, so the theory had to gain support in other ways.
One solution that Einstein immediately arrived at was to explain an anomaly
in the orbit of Mercury. For years, it had been known that Newtonian grav-
ity wasn't quite matching up with astronomers' observations of Mercury's
path around the sun. By taking into account the effects of relativity's curved
_ Chapter 6: Revolutionizing Space and Time: Einstein's Relativity yj
space-time, Einstein's solution precisely matched the path observed by
astronomers.
Still, this wasn't quite enough to win over all the critics, because another
theory of gravity had its own appeal.
Putted in another direction: Einstein's
competition for a theory of qratfity
A couple of years before Einstein completed his theory of general relativity,
the Finnish physicist Gunnar Nordstrom introduced his metric theory of grav-
ity that also combined gravity with special relativity. He went further, taking
James Clerk Maxwell's electromagnetic theory and applying an extra space
dimension, which meant that the electromagnetic force was also included in
the theory. It was simpler and more comprehensive than Einstein's general
relativity, but ultimately wrong (in a way that most physicists then and today
see as fairly obvious). But this was the first attempt to use an extra dimen-
sion in a unification theory, so it's worth investigating a bit.
Einstein himself was supportive of Nordstrom's work to incorporate special
relativity with gravity. In a 1913 speech on the state of unifying the two, he
said that only his work and that of Nordstrom met the necessary criteria.
In 1914, though, Nordstrom introduced a mathematical trick that increased
the stakes of unification. He took Maxwell's electromagnetic equations and
formulated them in four space dimensions, instead of the usual three that
Einstein had used. The resulting equations included the equation describing
the force of gravity!
Including the dimension of time, this made Nordstrom's theory a
5-dimensional space-time theory of gravity. He treated our universe as
a 4-dimensional projection of a 5-dimensional space-time. (This is kind of
similar to how your shadow on a wall is a 2-dimensional projection of your
3-dimensional body.) By adding an extra dimension to an established physi-
cal theory, Nordstrom unified electromagnetics and gravity! This provides an
early example of a principle from string theory — that the addition of extra
dimensions can provide a mathematical means for unifying and simplifying
physical laws.
When Einstein published his complete theory of general relativity in 1915,
Nordstrom jumped ship on his own theory because Einstein could explain
Mercury's orbit while his own theory could not.
Nordstrom's theory had a lot going for it, though, because it was much sim-
pler than Einstein's theory of gravity. In 1917, a year after Nordstrom himself
had given up on it, some physicists considered his metric theory a valid alter-
native to general relativity. Nothing noteworthy came out of these scientists'
efforts, though, so clearly they had backed the wrong theory.
y If Part II: The Physics Upon Which String Theory Is Built _
The eclipse that confirmed Einstein's fife Work
One major difference between Einstein's and Nordstrom's theories was that
they made different predictions about light's behavior. Under Nordstrom's
theory, light always traveled in a straight line. According to general relativity,
a beam of light would curve within a gravitational field.
In fact, as early as the late 1700s, physicists had predicted that light would
curve under Newtonian gravity. Einstein's equations showed that these ear-
lier predictions were off by a factor of 2.
The deflection of light predicted by Einstein is due to the curvature of space-time
around the sun. Because the sun is so massive that it causes space-time to curve,
a beam of light that travels near the sun will travel along a curved path — the
"shortest" path along the curved space-time, as shown in Figure 6-7.
In 1911, Einstein had done enough work on general relativity to predict how
much the light should curve in this situation, which should be visible to
astronomers during an eclipse.
Astronomers on an expedition to Russia in 1914 attempted to observe the
deflection of light by the sun, but the team ran into one little snag: World War I.
Arrested as prisoners of war and released a few weeks later, the astronomers
missed the eclipse that would have tested Einstein's theory of gravity.
This turned out to be great news for Einstein, because his 1911 calculations
contained an error! Had the astronomers been able to view the eclipse in
1914, the negative results might have caused Einstein to give up his work on
general relativity.
_ Chapter 6: Revolutionizing Space and Time: Einstein's Relativity y J?
When he published his complete theory of general relativity in 1915, he'd
corrected the problem, making a slightly modified prediction for how the
light would be deflected. In 1919, another expedition set out, this time to the
west African island of Principe. The expedition leader was British astronomer
Arthur Eddington, a strong supporter of Einstein.
Despite hardships on the expedition, Eddington returned to England with the
pictures he needed, and his calculations showed that the deflection of light
precisely matched Einstein's predictions. General relativity had made a pre-
diction that matched observation.
Albert Einstein had successfully created a theory that explained the gravita-
tional forces of the universe and had done so by applying a handful of basic
principles. To the degree possible, the work had been confirmed, and most of
the physics world agreed with it.
Almost overnight, Einstein's name became world famous. In 1921, Einstein
traveled through the United States to a media circus that probably wasn't
matched until the Beatlemania of the 1960s.
Applying Einstein's Work to the
Mysteries of the Universe
Einstein's work in developing the theory of relativity had shown amazing
results, unifying key concepts and clarifying important symmetries in the uni-
verse. Still, there are some cases where relativity predicts strange behavior,
such as singularities, where the curvature of space-time becomes infinite and
the laws of relativity seem to break down. String theory today continues this
work by trying to extend the concepts of relativity into these areas, hoping to
find new rules that work in these regions.
With relativity in place, physicists could look to the heavens and begin
a study of how the universe evolved over time, a field called cosmology.
However, Einstein's field equations also allow for some strange behavior —
such as black holes and time travel — that has caused great distress to
Einstein and others over the years.
If you haven't read about relativity before, this chapter may seem like a whirl-
wind of strange, exotic concepts — and these new theories certainly felt so
to the physicists of the time. Fundamental concepts — motion, mass, energy,
space, time, and gravity — were transformed in a period of only 15 years!
Motion, instead of being just some incidental behavior of objects, was now
crucial to understanding how the laws of physics manifested themselves.
The laws don't change — this was key to all of Einstein's work — but they
96
Part II: The Physics Upon Which String Theory Is Built _
can manifest in different ways, depending on where you are and how you're
moving — or how space-time is moving around you.
In Chapter 9, 1 cover the ideas of modern cosmology arising from Einstein's
work, such as the black holes that can form when massive quantities of
mass cause space-time to curve infinitely far and similar problems that come
up when trying to apply relativity to the early universe. Or, as you see in
Chapter 16, some solutions to Einstein's equations allow time travel.
Einstein himself was extremely uncomfortable with these unusual solutions
to his equations. To the best of his ability, he tried to disprove them. When
he failed, he would sometimes violate his own basic belief in the mathematics
and claim that these solutions represented physically impossible situations.
Despite the strange implications, Einstein's theory of general relativity has
been around for nearly a century and has met every challenge — at least
when applied to objects larger than a molecule. As 1 point out in Chapter 2,
at very small scales quantum effects become important, and the descrip-
tion using general relativity begins to break down. The equations make no
sense, and space-time becomes an exotic, tumultuous mess of energy fluctua-
tions. The force of gravity explodes to an infinite value. String theory (hope-
fully) represents one way of reconciling gravity at this realm, as I explain in
Chapters 10 and 11.
Katuza-Ktein Theory — String
Theory's Predecessor
One of the earliest attempts to unify gravity and electromagnetic forces came
in the form of Kaluza-Klein theory, a short-lived theory that again unified the
forces by introducing an extra space dimension. In this theory, the extra
space dimension was curled up to a microscopic size. Though it failed, many
of the same concepts were eventually applied in the study of string theory.
Einstein's theory had proved so elegant in explaining gravity that physicists
wanted to apply it to the other force known at the time — the electromagnetic
force. Was it possible that this other force was also a manifestation of the
geometry of space-time?
In 1915, even before Einstein completed his general relativity field equations,
the British mathematician David Hilbert said that research by Nordstrom and
others indicated "that gravitation and electrodynamics are not really differ-
ent." Einstein responded, "I have often tortured my mind in order to bridge
the gap between gravitation and electromagnetism."
_ Chapter 6: Revolutionizing Space and Time: Einstein's Relativity y /
One theory in this regard was developed and presented to Einstein in 1919
by German mathematician Theodor Kaluza. In 1914, Nordstrom had written
Maxwell's equations in five dimensions and had obtained the gravity equa-
tions (see the section "Pulled in another direction: Einstein's competition for
a theory of gravity"). Kaluza took the gravitational field equations of general
relativity and wrote them in five dimensions, obtaining results that included
Maxwell's equations of electromagnetism!
When Kaluza wrote to Einstein to present the idea, the founder of relativ-
ity replied by saying that increasing the dimensions "never dawned on
me" (which means he must have been unaware of Nordstrom's attempt to
unify electromagnetism and gravity, even though he was clearly aware of
Nordstrom's theory of gravity).
In Kaluza's view, the universe was a 5-dimensional cylinder and our
4-dimensional world was a projection on its surface. Einstein wasn't quite
ready to take that leap without any evidence for the extra dimension. Still, he
incorporated some of Kaluza's concepts into his own unified field theory that
he published and almost immediately recanted in 1925.
A year later, in 1926, Swedish physicist Oskar Klein dusted off Kaluza's theory
and reworked it into the form that has come to be known as the Kaluza-Klein
theory. Klein introduced the idea that the fourth space dimension was rolled
up into a tiny circle, so small that there was essentially no way for us to
detect it directly.
In Kaluza-Klein theory, the geometry of this extra, hidden space dimension
dictated the properties of the electromagnetic force — the size of the circle,
and a particle's motion in that extra dimension, related to the electrical
charge of a particle. The physics fell apart on this level because the predic-
tions of an electron's charge and mass never worked out to match the true
value. Also, many physicists initially intrigued with the Kaluza-Klein theory
became far more intrigued with the growing field of quantum mechanics,
which had actual experimental evidence (as you see in Chapter 7).
Another problem with the theory is that it predicted a particle with zero
mass, zero spin, and zero charge. Not only was this particle never observed
(despite the fact that it should have been, because it's a low-energy particle),
but the particle corresponded to the radius of the extra dimensions. It didn't
make sense to add a theory with extra dimensions and then have a result be
that the extra dimensions effectively didn't exist.
There is another (though less conventional) way to describe the failure of
Kaluza-Klein theory, viewing it as a fundamental theoretical limitation: For
electromagnetism to work, the extra dimension's geometry had to be com-
pletely fixed.
y $ Part II: The Physics Upon Which String Theory Is Built _
In this view, tacking an extra dimension onto a theory of dynamic space
should result in a theory that is still dynamic. Having a fifth dimension that's
fixed (while the other four dimensions are flexible) just doesn't make sense
from this point of view. This concept, called background dependence, returns
as a serious criticism of string theory in Chapter 17.
Whatever the ultimate reason for its failure, Kaluza-Klein theory lasted for
only a short time, although there are indications that Einstein continued to
tinker with it off and on until the early 1940s, incorporating elements into his
various failed unified field theory attempts.
In the 1970s, as physicists began to realize that string theory contained extra
dimensions, the original Kaluza-Klein theory served as an example from the
past. Physicists once again curled up the extra dimensions, as Klein had
done, so they were essentially undetectable (I explain this in more detail in
Chapter 10). Such theories are called Kaluza-Klein theories.
Chapter 7
Brushing Up on Quantum
Theory Basics
In This Chapter
Exploring the early days of quantum physics
Riding a wave of new ideas about light and particles
Realizing that some quantities can't be measured precisely
Considering different models of quantum physics
Scaling Planck units down (or up) to size
1\ s strange as relativity may have seemed to you (see Chapter 6), it's a
r • cakewalk compared to understanding quantum physics. In this strange
realm of physics — the realm of the extremely small — particles don't have
definite positions or energies. They can exist not only as particles, but also
as waves, but only when you don't look at them. One hope scientists have is
that string theory will explain some of the unusual results in quantum physics
or, at the least, reconcile it with general relativity. Particle physics, on the
other hand, is at the heart of string theory's origins and is a direct consequence
of this early work in quantum physics (see Chapter 8). Without quantum
physics, string theory could not exist.
As in the other chapters in this part, the goal of this chapter is not to provide a
complete overview of all of quantum physics — there are other books that do
a fine job of that, including Quantum Physics For Dummies by Steven Holzner
(Wiley). My goal here is to give you the background you need to know about
quantum physics so you can understand certain aspects of string theory.
It may not seem that these ideas relate directly to string theory, but being
familiar with these concepts will be handy down the road when I explain
string theory itself.
7 00 Part " : The Physics Upon Which String Theory Is Built _
In this chapter, I give you a brief introduction to the history and principles
of quantum physics, just enough so you can understand the later concepts
related to string theory. I explain how quantum theory allows objects to act
as both particles and waves. You explore the implications of the uncertainty
principle and probability in quantum physics (dead cat not required). I list
some of the many interpretations of what all of these strange quantum rules
may actually mean — though no one really knows (or can know) for sure.
Finally, I discuss the idea that special natural units can be used to describe
reality.
Unlocking the First Quanta: The
Birth of Quantum Physics
Quantum physics traces its roots back to 1900, when German physicist
Max Planck proposed a solution to a thermodynamics problem — a problem
having to do with heat. He resolved the problem by introducing a mathematical
trick — if he assumed that energy was bundled in discrete packets, or quanta,
the problem went away. (It proved to be brilliant because it worked. There
was no theoretical reason for doing this, until Einstein came up with one five
years later, as discussed in the next section.) In the process of doing this,
Planck used a quantity known as Planck's constant, which has proved essential
to quantum physics — and string theory.
Planck used this quantum concept — the concept that many physical
quantities come in discrete units — to solve a problem in physics, but even
Planck himself assumed that this was just a clever mathematical process to
remove the infinity. It would take five years for Albert Einstein to continue
the quantum revolution in physics.
The blackbody radiation problem, which Planck was trying to solve, is a
basic thermodynamics problem where you have an object that is so hot that
it glows inside. A small hole allows the light to escape, and it can be studied.
The problem is that in the 1800s, experiments and theories in this area didn't
match up.
A hot object radiates heat in the form of light (hot coals in a fire or the metal
rings on electric stoves are both good examples of this). If this object were
open inside, like an oven or a metal box, the heat would bounce around
inside. This sort of object was called a blackbody — because the object itself
doesn't reflect light, only radiates heat — and throughout the 1800s, various
theoretical work in thermodynamics had examined the way heat behaved
inside a blackbody.
.Chapter 7: Brushing Up on Quantum Theory Basics / (/ /
Now assume that there's a small opening — like a window — in the oven,
through which light can escape. Studying this light reveals information about
the heat energy within the blackbody.
Essentially, the heat inside a blackbody took the form of electromagnetic
waves, and because the oven is metal, they're standing waves, with nodes
where they meet the side of the oven (see Chapter 5 for details about
waves). This fact — along with an understanding of electromagnetics and
thermodynamics — can be used to calculate the relationship between light's
intensity (or brightness) and wavelength.
The result is that as the wavelength of light gets very small (the ultraviolet
range of electromagnetic energy), the intensity is supposed to increase
dramatically, approaching infinity.
In nature, scientists never actually observe infinities, and this was no
exception (see Chapter 2 for more about infinities). The research showed
that there were maximum intensities in the ultraviolet range, which completely
contradicted the theoretical expectations, as shown in Figure 7-1. This
discrepancy came to be known as the ultraviolet catastrophe.
^— ^— 1.2
Figure 7-1: _ 1.0 -
The ultra- ■£
violet ~
catastrophe '«
occurred 3
when theory —
and experi-
ment didn't
match in
studying
blackbody
radiation.
\Theoretical prediction
(5000 K)
1500 2000 2500
Wavelength (nm)
The ultraviolet catastrophe threatened to undermine the theories of
electromagnetics and/or thermodynamics. Clearly, if they didn't match
experiment, then one or both of the theories contained errors.
/ Q2 Part I': The Physics Upon Which String Theory Is Built _
When Planck resolved the ultraviolet catastrophe in 1900, he did so by
introducing the idea that the atom could only absorb or emit light in quanta
(or discrete bundles of energy). One implication of this radical assumption
was that there would be less radiation emitted at higher energies. By
introducing the idea of discrete energy packets — by quantizing energy —
Planck produced a solution that resolved the situation without having to
dramatically revise the existing theories (at least at that time).
Planck's insight came when he looked at the data and tried to figure out
what was going on. Clearly, the long wavelength predictions were close
to matching with experiment, but the short wavelength light was not. The
theory was over-predicting the amount of light that would be produced at
short wavelengths, so he needed a way to limit this short wavelength.
Knowing some things about waves, Planck knew that the wavelength and
frequency were inversely related. So if you're talking about waves with short
wavelength, you're also talking about waves with high frequency. All he had
to do was find a way to lower the amount of radiation at high frequencies.
Planck reworked the equations, assuming that the atoms could only emit or
absorb energy in finite quantities. The energy and frequency were related
by a proportion called Planck's constant. Physicists use the variable h to
represent Planck's constant in his resulting physics equations.
The resulting equation worked to explain the experimental results of
blackbody radiation. Planck, and apparently everyone else, thought this was
just a mathematical sleight of hand that had resolved the problem in one
strange, special case. Little did anyone realize that Planck had just laid the
foundation for the strangest scientific discoveries in the history of the world.
Fun With Photons: Einstein's
Nobel Idea of Liqht
Einstein received the Nobel Prize not for relativity, but instead for his work
in using Planck's idea of the quantum to explain another problem — the
photoelectric effect. He went further than Planck, suggesting that all
electromagnetic energy was quantized. Light, Einstein said, moved not in
waves, but in packets of energy. These packets of energy became called
photons. Photons are one of the fundamental particles of physics that
physicists hope to explain using string theory.
_ Chapter 7: Brushing Up on Quantum Theory Basics / (}j
Powered by the photoelectric effect
Modern solar cells work off the same principle run through wires to create an electric current
as the photoelectric effect. Composed of photo- that can power devices such as ornamental
electric materials, they take electromagnetic lights in your flowerbed or NASA's Martian
radiation in the form of sunlight and convert it rovers,
into free electrons. Those free electrons then
The photoelectric effect occurs when light shines on certain materials that
then emit electrons. It's almost as if the light knocks loose the electrons,
causing them to fly off the material. The photoelectric effect was first
observed in 1887 by Heinrich Hertz, but it continued to puzzle physicists
until Einstein's 1905 explanation.
At first, the photoelectric effect didn't seem that hard to explain. The
electrons absorbed the light's energy, which caused the electrons to fly
off the metal plate. Physicists still knew very little about electrons — and
virtually nothing about the atom — but this made sense.
As expected, if you increased the light's intensity (the total energy per second
carried by the beam), more electrons definitely were emitted (see the top of
Figure 7-2). There were two unexpected problems though:
i^ Above a certain wavelength, no electrons are emitted — no matter how
(intense the light is (as shown in the bottom of Figure 7-2).
j-" When you increase the light's intensity, the speed of the electrons
doesn't change.
Einstein saw a connection between this first problem and the ultraviolet
catastrophe faced by Max Planck (see the preceding section for more about
Planck's work), but in the opposite direction. The longer wavelength light (or
light with lower frequency) failed to do things that were being achieved by
the shorter wavelength light (light with higher frequency).
Planck had created a proportional relationship between energy and frequency.
Einstein again did what he was best at — he took the mathematics at face
value and applied it consistently. The result was that the high frequency light
had higher energy photons, so it was able to transfer enough energy into the
electron for it to get knocked loose. The lower frequency photons didn't have
enough energy to help any electrons escape. The photons had to have energy
above a certain threshold to knock the electrons loose.
7 Ol} Part ll: The Physics Upon Which String Theory Is Built _
Similarly, the second problem of the noneffect of light's intensity on an
electron's speed is also solved by Einstein's quantum view of light. Each
photon's energy is based on its frequency (or wavelength), so increasing
the intensity doesn't change the energy of each photon; it only increases the
total number of photons. This is why increasing the intensity causes more
electrons to get emitted, but each electron maintains the same speed. The
individual photon knocks out an electron with the same energy as before, but
more photons are doing the same job. No single electron gets the benefit of
the increase in intensity.
Based on the principle that the speed of light was constant (the basis of his
special theory of relativity), Einstein knew that these photons would always
move at the same velocity, c. Their energy would be proportional to the
frequency of the light, based on Planck's definitions.
_ Chapter 7: Brushing Up on Quantum Theory Basics / (/f)
WaVes and Particles Living Together
Within quantum physics, two alternate explanations of light work, depending on
the circumstances. Sometimes light acts like a wave, and sometimes it acts
like a particle, the photon. As quantum physics continued to grow, this wave
particle duality would come up again and again, as even particles seemed to
begin acting like waves. The explanation for this strange behavior lies in the
quantum wavefunction, which describes the behavior of individual particles
in a wave-like way. This strange quantum behavior of particles and waves is
crucial to understanding quantum theories, such as string theory.
Einstein's theory of special relativity had seemingly destroyed the theory
of an ether medium, and with his theory of the photon he proved how light
could work without it. The problem was that for more than a century, there
had been proof that light did, indeed, act like a wave.
Light as a Watfe: The double
slit experiment
The experiment that proved that light acts like a wave was the double slit
experiment. It showed a beam of light passing through two slits in a barrier,
resulting in light and dark interference bands on a screen. This sort of
interference is a hallmark of wave behavior, meaning that light had to be in
the form of waves.
These interference patterns in light had been observed in Isaac Newton's
time, in the work of Francesco Maria Grimaldi. These experiments were
vastly improved upon by the young experimenter Thomas Young in 1802.
For the experiment to work, the light passing through the two slits needed to
have the same wavelength. Today, you can accomplish this with lasers, but
they weren't available in Young's day, so he came up with an ingenious way
to get a single wavelength. He created a single slit and let light pass through
that, and then that light went through two slits. Because the light passing
through the two slits came from the same source, they were in phase with
each other, and the experiment worked. This experimental setup is shown in
Figure 7-3.
106
Part II: The Physics Upon Which String Theory Is Built _
As you can see in the figure, the end result is a series of bright and dark
bands on the final screen. This comes from the interference of the light
waves, shown back in Figure 5-2 in Chapter 5. Recall that interference means
you add the amplitude of the waves. Where high and low amplitudes overlap,
they cancel each other out, resulting in dark bands. If high amplitudes
overlap, the amplitude of the total wave is the sum of them, and the same
happens with low amplitudes, resulting in the light bands.
This dual behavior was the problem facing Einstein's photon theory of
light, because though the photon had a wavelength, according to Einstein,
it was still a particle! How could a particle possibly have a wavelength?
Conceptually, it made no real sense, until a young Frenchman offered a
resolution to the situation.
Particles as a Watfe: The de Broqlie
hypothesis
In 1923, Frenchman Louis de Broglie proposed a bold new theory: Particles of
matter also had wavelengths and could behave as waves, just as photons did.
Here was de Broglie's line of reasoning. Under special relativity, matter and
energy were different manifestations of the same thing. The photon, a particle
of energy, had a wavelength associated with it. Therefore, particles of matter,
such as electrons, should also have wavelengths. His PhD dissertation set out
to calculate what that wavelength (and other wave properties) should be.
Two years later, two American physicists demonstrated de Broglie's experiment
by performing experiments that showed interference patterns with electrons,
as shown in Figure 7-4. (The 1925 experiment wasn't actually a double slit
experiment, but it showed the interference clearly. The double slit experiment
with electrons was conducted in 1961.)
_ Chapter 7: Brushing Up on Quantum Theory Basics / (//
Figure 7-4: k
Electrons U^^> :
demonstrate ^^^
interfer- Electron
ence
double slit
experiment.
the a""
^
This behavior showed that whatever quantum law governed photons also
governed particles. The wavelength of particles such as the electron is very
small compared to the photon. For larger objects, the wavelength is even
smaller still, quickly becoming so small as to become unnoticeable. This is
why this sort of behavior doesn't show up for larger objects. If you flung
baseballs through the two slits, you'd never notice an interference pattern.
Still, this left open the question of what was causing the wave behavior in
these particles of energy or matter. The answer would be at the core of the
new field of quantum mechanics. (String theory will later say that both types
of particles — matter and energy — are manifestations of vibrating strings,
but that's about 50 years down the road from de Broglie's time.)
You can picture the problem if you look at the way the experiment is set up
in Figure 7-5. The light wave passes through both slits, and that's why the
waves interfere with each other. But an electron — or a photon, for that
matter — cannot pass through both slits at the same time if you think of them
the way we're used to thinking of them; it has to pick a slit. In this classical
case (where the photon is a solid object that has a certain position), there
shouldn't be any interference. The beam of electrons should hit the screen
in one general spot, just as if you were throwing baseballs through a hole
against a wall. (This is why quantum physics challenges our classical thinking
about objects and was deemed so controversial in its early years.)
In fact, if you close one of the slits, this is exactly what happens. When a slit
is closed, the interference pattern goes away — the photons or electrons col-
lect in a single band that spreads out from the brightest spot at the center.
So the interference patterns can't be explained by particles bouncing off the
side of the slits or anything normal like that. It's a genuinely strange behavior
that required a genuinely strange solution — in the form of quantum mechanics.
/ QS Part I': The Physics Upon Which String Theory Is Built _
Quantum physics to the rescue:
The quantum Malfunction
The solution to the problem took the form of the quantum wavefunction,
developed by Erwin Schrodinger. In this function, the location of the particle
is dictated by a wave equation describing the probability of the particle's
existence at a given point, even though the particle has a definite location
when measured.
Schrodinger's wavefunction was based in part on his reading of de Broglie's
hypothesis about matter having a wavelength. He used this behavior to
analyze atomic models created by Niels Bohr (which I cover in Chapter 8).
The resulting wavefunction explained the behavior of these atoms in terms
of waves. (Bohr's student, Werner Heisenberg, had come up with a different
mathematical representation to solve the atomic problem. Heisenberg's
matrix method was later shown to be mathematically equivalent to
Schrodinger's wavefunction. This sort of parallel work comes up often in
physics, as you'll see in Chapters 10 and 11 about the development of string
theory.)
The wavefunction created the wave behavior. In this viewpoint, the wave
passed through both slits, even though no single, classical individual particle
could pass through both slits. The wavefunction, which describes the
probability of the particle arriving at a point, can be thought of as passing
through both slits and creating the interference pattern. This is an interference
pattern of probabilities, even though the particles themselves end up having a
definite location (and therefore must pass through one slit).
_ Chapter 7: Brushing Up on Quantum Theory Basics / (/y
Still, this isn't the end of the odd story of the double slit experiment. The
strange dual behavior — wave and particle — was still there. But now a
mathematical framework existed that allowed physicists to talk about the
duality in a manner that made some sort of mathematical sense. The theory
still held many more mysteries to be uncovered.
Whu We Can't Measure It Alt:
The Uncertainty Principle
Werner Heisenberg is best known in quantum physics for his discovery of
the uncertainty principle, which states that the more precisely you measure
one quantity, the less precisely you can know another associated quantity.
The quantities sometimes come in set pairs that can't both be completely
measured. One consequence of this is that to make measurements of very
short distances — such as those required by string theory — very high
energies are required.
What Heisenberg found was that the observation of a system in quantum
mechanics disturbs the system enough that you can't know everything about
the system. The more precisely you measure the position of a particle, for
example, the less it's possible to precisely measure the particle's momentum.
The degree of this uncertainty was related directly to Planck's constant —
the same value that Max Planck had calculated in 1900 in his original quantum
calculations of thermal energy. (You'll shortly see that Planck's constant has
a lot of unusual implications.)
Heisenberg found that certain complementary quantities in quantum physics
were linked by this sort of uncertainty:
(-" Position and momentum (momentum is mass times velocity)
v" Energy and time
This uncertainty is a very odd and unexpected result from quantum
physics. Until this time, no one had ever made any sort of prediction that
knowledge was somehow inaccessible on a fundamental level. Sure, there
were technological limitations to how well a measurement was made, but
Heisenberg's uncertainty principle went further, saying that nature itself
doesn't allow you to make measurements of both quantities beyond a certain
level of precision.
/ / Part ll: The Physics Upon Which String Theory Is Built _
One way to think about this is to imagine that you're trying to observe a
particle's position very precisely. To do so, you have to look at the particle.
But you want to be very precise, which means you need to use a photon with
a very short wavelength, and a short wavelength relates to a high energy. If
the photon with high energy hits the particle — which is exactly what you
need to have happen if you want to observe the particle's position precisely —
then it's going to give some of its energy to the particle. This means that any
measurement you also try to make of the particle's momentum will be off. The
more precisely you try to measure the position, the more you throw off your
momentum measurement!
Similar explanations work if you observe the particle's momentum precisely,
so you throw off the position measurement. The relationship of energy and
time has a similar uncertainty. These are mathematical results that come
directly out of analyzing the wavefunction and the equations de Broglie used
to describe his waves of matter.
How does this uncertainty manifest in the real world? For that, let me return
to your favorite quantum experiment — the double slit. The double slit
experiment has continued to grow odder over the years, yielding stranger
and stranger results. For example:
j"* If you send the photons (or electrons) through the slits one at a time,
the interference pattern shows up over time (recorded on a film), even
though each photon (or electron) has seemingly nothing to interfere with.
i^ If you set up a detector near either (or both) slits to detect which slit the
photon (or electron) went through, the interference pattern goes away.
J-" If you set up the detector but leave it turned off, the interference pattern
comes back.
W If you set up a means of determining later what slit the photon (or
electron) went through, but do nothing to impact it right now, the
interference pattern goes away.
What does all of this have to do with the uncertainty principle? The common
denominator among the cases where the interference pattern goes away is
that a measurement was made on which slit the photons (or electrons) passed
through.
When no slit measurement is made, the uncertainty in position remains high,
and the wave behavior appears dominant. As soon as a measurement is
made, the uncertainty in position drops significantly and the wave behavior
vanishes. (There is also a case where you observe some of the photons or
electrons. Predictably, in this case, you get both behaviors, in exact ratio to
how many particles you're measuring.)
.Chapter 7: Brushing Upon Quantum Theory Basics f f f
Dead Cats, Live Cats, and Probability
in Quantum Physics
In the traditional interpretation of quantum physics, the wavefunction is seen
as a representation of the probability that a particle will be in a given location.
After a measurement is made, the wavefunction collapses, giving the particle
a definite value for the measured quantity.
In the double slit experiments, the wavefunction splits between the two
slits, and this wavefunction results in an interference of probabilities on the
screen. When the measurements are made on the screen, the probabilities
are distributed so that it's more likely to find particles in some places and
less likely to find them in other places, resulting in the light and dark
interference bands. The particle never splits, but the probability of where the
particle will be does split. Until the measurement is made, the distribution of
probabilities is all that exists.
This interpretation was developed by the physicist Max Born and grew to be
the core of the Copenhagen interpretation of quantum mechanics (which I
explain toward the end of this chapter). For this explanation, Born received
(three decades later) the 1954 Nobel Prize in Physics.
Almost as soon as the explanation of probabilities was proposed, Erwin
Schrodinger came up with a morbid thought experiment intended to show
how absurd it was. It's become one of the most important, and misunderstood,
concepts in all of physics: the Schrodinger's cat experiment.
In this experiment, Schrodinger hypothesized a radioactive particle that has
a 50 percent chance of decaying within an hour. He proposed that you place
the radioactive material within a closed box next to a Geiger counter that
would detect the radiation. When the Geiger counter detects the radiation
from the decay, it will break a glass of poison gas. Also inside the box is a cat.
If the glass breaks, the cat dies. (I told you it was morbid.)
Now, according to Born's interpretation of the wavefunction, after an hour
the atom is in a quantum state where it is both decayed and not decayed —
50 percent chance of each result. This means the Geiger counter is in a state
where it's both triggered and not triggered. The glass containing the poison
gas is both broken and not broken. The cat is both dead and alive!
This may sound absurd, but it's the logical extension of the particle being
both decayed and not decayed. Schrodinger believed that quantum physics
couldn't describe such an insane world, but that the cat had to be either
completely alive or completely dead even before the box is opened and
observed.
7 72 Part ll: The Physics Upon Which String Theory Is Built _
After you open the box, according to this interpretation, the cat's state
becomes well defined one way or the other, but in the absence of a
measurement, it's in both states. Though Schrodinger's cat experiment was
created to oppose this interpretation of quantum mechanics, it has become
the most dramatic example used to illustrate the strange quantum nature of
reality.
Does Anyone Know What Quantum
Theory Means}
Quantum physics is based on experimental evidence, much of which was
obtained in the first half of the 20th century. The odd behavior has been
seen in laboratories around the world, continually agreeing with the theory,
despite all common sense. The really strange behavior occurs only on small
scales; when you get to the size of cats, the quantum phenomena seems to
always take on a definite value. Still, even today, the exact meaning of this
strange quantum behavior is up in the air — something that doesn't trouble
most modern physicists who work on these problems.
Some physicists hope that a "theory of everything," perhaps even string
theory, may provide clear explanations for the underlying physical meaning
of quantum physics. Among them, Lee Smolin has cited string theory's failure
to explain quantum physics as a reason to look elsewhere for a fundamental
theory of the universe — a view that is certainly not maintained by the
majority of string theorists. Most string theorists believe that what matters
is that quantum physics works (that is, it makes predictions that match
experiment) and the philosophical concerns of why it works are less
important. All of the interpretations of why quantum physics work yield the
same experimental predictions, so they are effectively equivalent.
Einstein spent the last 30 years of his life railing against the scientific and
philosophical implications of quantum physics. This was a lively time of
debate in physics, as he and Niels Bohr sparred back and forth. "God does
not play dice with the universe," Einstein was quoted as saying. Bohr replied,
"Einstein, stop telling God what to do!"
A similar era may be upon us now, as theoretical physicists attempt to
uncover the fundamental principles that guide string theory. Unlike quantum
theory, there are few (if any) experimental results to base new work on, but
there are many Einsteinian critics — again, on both scientific and philosophical
grounds. (We get to them in Part V.)
Even with a firm theory that clearly works, physicists continue to question
what quantum physics really means. What is the physical reality behind the
mathematical equations? What actually happens to Schrodinger's cat? Some
.Chapter 7: Brushing Upon Quantum Theory Basics / #3
physicists hope that string theory may provide an answer to this question,
though this is far from the dominant view. Still, any successful attempt to
extend quantum physics into a new realm could provide unexpected insights
that may resolve the questions.
Interactions transform quantum systems:
The Copenhagen interpretation
The Copenhagen interpretation represents the orthodox view of quantum
physics as it's taught in most undergraduate level courses, and it's mostly
how I've interpreted quantum physics in this chapter: An observation or
measurement causes the wavefunction to collapse from a general state of
probabilities to a specific state.
The name comes from the Copenhagen Institute in (you guessed it)
Copenhagen, Denmark, where Niels Bohr and his students helped form
quantum physics in the 1920s and early 1930s, before World War II caused
many to leave the Netherlands as they picked sides.
In today's talk, most physicists view the particles in the wavefunction as
continually interacting with the world around them. These interactions are
enough to cause the wavefunction to go through a process called decoherence,
which basically makes the wavefunction collapse into a definite value. In
other words, the very act of interacting with other matter causes a quantum
system to become a classical system. Only by carefully isolating the quantum
system to avoid such interactions will it remain in a coherent state, staying
as a wave long enough to exhibit exotic quantum behaviors such as interference.
Under this explanation, you don't have to open the box for Schrodinger's cat
to take on a definite state. The Geiger counter is probably where the breakdown
occurs, and reality makes a "choice" of whether the particle has or has not
decayed. Decoherence of the wavefunction takes place well before it ever
reaches the cat.
If no one's there to see it, does the universe
exist} The participatory anthropic principle
The participatory anthropic principle (PAP) was proposed by the physicist
John Archibald Wheeler when he said that people exist in a "participatory
universe." In Wheeler's (extremely controversial) view, an actual observer
is needed to cause the collapse of the wavefunction, not just bits and pieces
bouncing into each other.
/ / I) Part II: The Physics Upon Which String Theory Is Built _
This stance goes significantly further than the strict tenets of the
Copenhagen interpretation, but it can't be completely dismissed when you
look in depth at the quantum evidence. If you never look at the quantum
system, then for all intents and purposes it always stays a quantum system.
Schrodinger's cat really is both alive and dead until a person looks inside
the box.
To John Barrow and Frank Tipler (in their popular and widely controversial
1986 book The Anthropic Cosmological Principle), this means that the universe
itself comes into being only if someone is there to observe it. Essentially, the
universe requires some form of life present for the wavefunction to collapse
in the first place, meaning that the universe itself could not exist without life
in it.
Most physicists believe that the PAP approach places humans in a crucial
role in the universe, a stance which went out of favor when Copernicus
realized Earth wasn't the center of the universe. As such, they (rightly, I
believe) dismiss this interpretation in favor of those where humans aren't
necessary components of the universe.
This is an especially strong statement of a concept known as the anthropic
principle. Recent discoveries in string theory have caused some theoretical
physicists who were once strongly opposed to any form of anthropic principle
to begin to adopt weaker versions of the anthropic principle as the only
means of making predictions from the vast array of string theory possibilities. I
explain more about this concept in Chapter 11.
All possibilities take place: The many
Worlds interpretation
In contrast, the many worlds interpretation (MWI) of Hugh Everett III proposes
that the wavefunction never actually collapses, but all possibilities become
actualities — just in alternate realities. The universe is continually splitting
apart as every quantum question is resolved in every possible way across an
immense multiverse of parallel universes.
This is one of the most unusual concepts to come out of quantum physics,
but it has its own merit. Like the work of Einstein described in Chapter 6,
Everett arrived at this theory in part by taking the mathematics of quantum
theory and assuming it could be taken literally. If the equation shows that
there are two possibilities, then why not assume that there are two possibilities?
.Chapter 7: Brushing Upon Quantum Theory Basics / / f)
When you look inside the box, instead of something odd happening to the
quantum system, you actually become part of the quantum system. You now
exist in two states — one state that has found a dead cat and one state that
has found a living cat.
^jjjABEfl Though these parallel universes sound like the stuff of science fiction, a related
' /^~^\ concept of parallel universes may arise as a prediction of string theory. In
Ulljl ) fact, it's possible that there are a vast number of parallel universes — a vast
multiverse. More on this in Chapter 15.
What are the odds) Consistent histories
In the consistent histories view, the many worlds aren't actually realized,
but the probability of them can be calculated. It eliminates the need for
observers by assuming that the infinite complexity of the universe can't be
fully dealt with, even mathematically, so it averages out over a large number
of possible histories to arrive at the probabilities of the ones that are more
probable, including the one universe that contains the outcome actually
witnessed — our own.
Strictly speaking, the consistent history interpretation doesn't exclude the
multiple worlds interpretation, but it only focuses on the one outcome you're
sure of, rather than the infinite outcomes that you can only conjecture.
From a physical standpoint, this is similar to the idea of decoherence. The
wavefunctions continually interact with particles just enough to keep all the
possibilities from being realized. After you analyze all the possible paths,
many of them cancel out, leaving only a couple of possible histories — the
cat is either alive or dead. Making the measurement determines which one is
the real history and which one was only a possibility.
Searching for more fundamental data:
The hidden Variables interpretation
One final interpretation is the hidden variables interpretation, where the
equations of quantum theory are hiding another level of physical reality.
The strange probabilities of quantum physics (under this explanation) are
the result of our ignorance. If you understood this hidden layer, the system
would be fully deterministic. (In other words, if you knew all the variables,
you'd know exactly what was going to happen, and the quantum probabilities
would go away.)
116
Part II: The Physics Upon Which String Theory Is Built _
The first hidden variables theory was developed in the 1920s by Louis de
Broglie, but a 1932 proof by John von Neumann showed that such theories
couldn't exist in quantum physics. In 1952, physicist David Bohm used a
mistake in this proof and reworked de Broglie's theory into his own variant
(which has become the most popular version).
The core of Bohm's argument was a mathematical counterexample to the
uncertainty principle, showing that quantum theory could be consistent with
the existence of particles that had definite position and velocity. He assumed
that these particles reproduced (on average) the results of the Schrodinger
wavefunction. He was then able to construct a quantum potential wave that
could guide the particles to behave in this way.
In Bohm's hidden variables theory, there is another hidden layer of physical
law that is more fundamental than quantum mechanics. The quantum
randomness would be eliminated if this additional layer could be understood.
If such a hidden layer exists, it should, in principle, be possible for physics to
someday reveal it in some way — perhaps through a "theory of everything."
(Of course, the existence of either a "hidden layer" or "theory of everything"
are ideas that aren't believed by most physicists today.)
Quantum Units of Nature — Planck Units
Physicists occasionally use a system of natural units, called Planck units,
which are calculated based on fundamental constants of nature like Planck's
constant, the gravitational constant, and the speed of light.
Planck's constant comes up often in discussing quantum physics. In fact, if
you were to perform the mathematics of quantum physics, you'd find that
little h variable all over the place. Physicists have even found that you can
define a set of quantities in terms of Planck's constant and other fundamental
constants, such as the speed of light, the gravitational constant, and the
charge of an electron.
These Planck units come in a variety of forms. There is a Planck charge and
a Planck temperature, and you can use various Planck units to derive other
units such as the Planck momentum, Planck pressure, and Planck force . . .
well, you get the idea.
For the purposes of the discussion of string theory, only a few Planck units are
relevant. They are created by combining the gravitational constant, the speed
of light, and Planck's constant, which makes them the natural units to use
when talking about phenomena that involve those three constants, such as
quantum gravity. The exact values aren't important, but here are the general
scales of the relevant Planck units:
_ Chapter 7: Brushing Up on Quantum Theory Basics / / /
j-" Planck length: 10 -35 meters (if a hydrogen atom were as big as our
galaxy, the Planck length would be the size of a human hair)
j-" Planck time: 10~ 43 seconds (the time light takes to travel the Planck
length — a very, very short period of time)
J-" Planck mass: 10~ 8 kilograms (about the same as a large bacteria or very
small insect)
w Planck energy: 10 28 electronvolts (roughly equivalent to a ton of TNT
explosive)
Keep in mind that the exponents represent the number of zeroes, so the
Planck energy is a 1 followed by 28 zeroes, in electronvolts. The most
powerful particle accelerator on Earth, the Large Hadron Collider that came
online briefly in 2008 can produce energy only in the realm of TeV — that is, a
1 followed by 12 zeroes, in electronvolts.
The negative exponents, in turn, represent the number of decimal places in
very small numbers, so the Planck time has 42 zeroes between the decimal
point and the first non-zero digit. It's a very small amount of time!
Some of these units were first proposed in 1899 by Max Planck himself,
before either relativity or quantum physics. Such proposals for natural units —
units based on fundamental constants of nature — had been made at least
as far back as 1881. Planck's constant makes its first appearance in the
physicist's 1899 paper. The constant would later show up in his paper on the
quantum solution to the ultraviolet catastrophe.
Planck units can be calculated in relation to each other. For example, it
takes exactly the Planck time for light to travel the Planck length. The
Planck energy is calculated by taking the Planck mass and applying Einstein's
E = mc 2 (meaning that the Planck mass and Planck energy are basically two
ways of writing the same value).
In quantum physics and cosmology, these Planck units sneak up all the time.
Planck mass represents the amount of mass needed to be crammed into the
Planck length to create a black hole. A field in quantum gravity theory would
be expected to have a vacuum energy with a density roughly equal to one
Planck energy per cubic Planck length — in other words, it's 1 Planck unit of
energy density.
Why are these quantities so important to string theory?
The Planck length represents the distance where the smoothness of relativity's
space-time and the quantum nature of reality begin to rub up against each
other. This is the quantum foam I explain in Chapter 2. It's the distance where
the two theories each, in their own way, fall apart. Gravity explodes to become
incredibly powerful, while quantum fluctuations and vacuum energy run
rampant. This is the realm where a theory of quantum gravity, such as string
theory, is needed to explain what's going on.
/ / S Part I': The Physics Upon Which String Theory Is Built _
Planck units and Zeno's paradox
If the Planck length represents the shortest
distance allowed in nature, it could be used to
solve the ancient Greek puzzle called Zeno's
paradox. Here is the paradox:
You want to cross a river, so you get in your
boat. To reach the other side, you must cross
half the river. Then you must cross half of
what's left. Now cross half of what's left. No
matter how close you get to the other side of
the river, you will always have to cover half
that distance, so it will take you forever to get
across the river, because you have to cross an
infinite number of halves.
The traditional way to solve this problem is with
calculus, where you can show that even though
there are an infinite number of halves, it's
possible to cross them all in a finite amount of
time. (Unfortunately for generations of stymied
philosophers, calculus was invented by Newton
and Leibnitz 2,000 years after Zeno posed his
problem.)
As it turns out, during my sophomore year I
solved Zeno's paradox in my calculus course
the same semester that I learned about Planck
units in my modern physics course. It occurred
to me that if the Planck length were really
the shortest distance allowed by nature, the
quantum of distance, it offered a physical
resolution to the paradox.
In my view, when your distance from the
opposite shore reaches the Planck length, you
can't go half anymore. Your only options are to
go the whole Planck length or go nowhere. In
essence, I pictured you "slipping" along that
last tiny little bit of space without ever actually
cutting the distance in half.
When I first came up with this idea as an
undergraduate physics major, I was extremely
impressed with myself. I have since learned
that I'm not the only person to have come up
with this connection between Planck length
and Zeno's paradox. Despite that, I'm still
somewhat impressed with myself.
In some sense, these units are sometimes considered to be quantum quantities
of time and space, and perhaps some of the other quantities as well. Mass
and energy clearly come in smaller scales, but time and distance don't seem
to get much smaller than the Planck time and Planck length. Quantum
fluctuations, due to the uncertainty principle, become so great that it
becomes meaningless to even talk about something smaller. (See the
nearby sidebar "Planck units and Zeno's paradox.")
In most string theories, the length of the strings (or length of compactified
extra space dimensions) are calculated to be roughly the size of the Planck
length. The problem with this is that the Planck length and the Planck energy
are connected through the uncertainty principle, which means that to explore
the Planck length — the possible length of a string in string theory — with
precision, you'd introduce an uncertainty in energy equal to the Planck energy.
This is an energy 16 orders of magnitude (add 16 zeroes!) more powerful than
the newest, most powerful particle accelerator on Earth can reach. Exploring
such small distances requires a vast amount of energy, far more energy than
we can produce with present technology.
Chapter 8
The Standard Model of
Particle Physics
In This Chapter
Accepting the atom and examining its parts
Applying quantum physics to the atom's bits and pieces
Categorizing particles into bosons and fermions
Using the Standard Model to reveal four forces of physics
Pondering the range of energies and masses observed
m Muring the mid-1900s, physicists further explored the foundations of
W>f quantum physics and the components of matter. They focused on the
study of particles in a field that became known as particle physics. More of
these itty-bitty particles seemed to spring up every time physicists looked for
them! By 1974, physicists had determined a set of rules and principles called
the Standard Model of particle physics — a model that includes all interactions
except for gravity.
Here I explore the Standard Model of particle physics and how it relates to
string theory. Any complete string theory will have to include the features
of the Standard Model and also extend beyond it to include gravity as well.
In this chapter, I describe the structure of the atom, including the smaller
particles contained within it, and the scientific methods used to explain the
interactions holding matter together. I identify the two categories of particles
that exist in our universe, fermions and bosons, and the different rules they
follow. Finally, I point out the problems that remain from the Standard Model,
which string theory hopes to resolve.
The topics related to the development of the Standard Model of particle
physics are detailed and fascinating in their own right, but this book is about
string theory. So my review of the material in this chapter is necessarily
brief and is in no way intended to be a complete look at the subject. Many
of the initial topics regarding the discovery of the structure of the atom are
recounted in Einstein For Dummies (Wiley), and many other popular books
are available to explore some of the more involved concepts of particle
physics that come along later.
/ 20 Part H: The Physics Upon Which String Theory Is Built _
Atoms, Atoms, Everywhere Atoms:
Introducing Atomic Theory
Physicist Richard P. Feynman once said that if he could boil down the most
important principles of physics to a single sentence, it would be, "All things
are made of atoms." (He actually goes on to expand on this, meaning that he
actually boiled physics down to a compound sentence. For our immediate
purposes, this first bit is enough.) The structure of atoms determines
fundamental properties of matter in our universe, such as how atoms
interact with each other in chemical combinations. The study of physics at
the scale of an atom is called atomic theory, or atomic physics. Though this is
several scales above the scale that string theory operates on, understanding
the smaller structure of matter requires some level of understanding of the
atomic-level structure.
Ancient Greeks considered the question of whether you could divide an object
forever. Some — such as the fifth century B.C. philosopher Democritus —
believed that you would eventually reach a smallest chunk of matter that
couldn't be divided any more, and they called these smallest chunks atoms.
Aristotle's view that matter was composed of five basic elements was
adopted by most philosophers of the time and remained the dominant way
of thinking for many years, well into the time that "natural philosophy" began
its transition into "science." After all, no scientists or philosophers had ever
seen a smallest chunk of matter, so there really wasn't any reason to suppose
they existed.
This began to change in 1738 when Swiss mathematician David Bernoulli
explained how pressurized gas behaved by assuming that gas was made up
of tiny particles. The heat of a gas was related to the speed of the particles.
(This built on the work of Robert Boyle, nearly a century earlier.)
In 1808, British chemist John Dalton tried to explain the behavior of
elements — substances that can't be chemically broken down into simpler
substances — by assuming that they were made up of atoms.
According to Dalton, each atom of an element was identical to other atoms of
the same element, and they combined together in specific ways to form the
more complex substances we see in our universe.
Over the next century, evidence for the atomic theory mounted (see the
sidebar "Einstein's contribution to atomic theory"). The complex structures
formed by different atoms were called molecules, though the exact mechanism
for how atoms formed molecules was still unclear.
.Chapter 8: The Standard Model of Particle Physics 727
Einstein's contribution to atomic theory
As if he weren't credited with enough, Albert
Einstein is also frequently cited as the person
who provided some of the last definitive
support for the atomic theory of matter in two of
his 1905 papers.
One of the papers was his PhD thesis, in which
he calculated the approximate mass of an atom
and the size of sugar molecules. This work
earned him his doctorate from the University of
Zurich.
The other paper involved analyzing random
motion in smoke and liquids. This type of motion
is called Brownian motion and had puzzled
physicists for some time. Einstein pictured the
motion as the result of atoms of smoke or liquid
being jostled around by atoms of the surrounding
gas or liquid, which explained the phenomenon
perfectly. His predictions were supported by
experimental findings.
It took more than 150 years from the time of Bernoulli for physicists to fully
adopt the atomic model. Then, as you find out in the next section, after it was
finally adopted, it was found to be incomplete! The complications arising in
the study of string theory may well prove to take just as long, and perhaps
ultimately be just as incomplete. But that doesn't mean they're necessarily
"wrong," any more than atomic theory is "wrong."
Popping Open the Atomic Hood
and Seeing What's Inside
Today scientists know that these atoms are not, as the Greeks imagined, the
smallest chunks of matter. Scientists quickly realized that atoms had multiple
parts inside of them:
IJ-" Negatively charged electrons circling the nucleus
J-" Positively charged nucleus
The particles that compose the nucleus (it's made up of smaller pieces, too)
and electrons are among the particles, along with several others, that the
Standard Model of particle physics explains, and ultimately that string theory
should also explain.
7 22 Part ll: The Physics Upon Which String Theory Is Built _
Discovering the electron
The electron is a negatively charged particle contained within the atom. It
was discovered in 1897 by British physicist J.J. Thomson, though charged
particles (including the name "electron") had been hypothesized earlier.
Some physicists had already hypothesized that units of charge might be
flowing around in electrical apparatus. (Benjamin Franklin proposed such an
idea as early as the 1700s.) Technology only caught up to this idea in the late
1800s, with the creation of the cathode ray tube, shown in Figure 8-1.
In a cathode ray tube, a pair of metal disks is connected to a battery. The
metal disks are placed inside a sealed glass tube that contains no air — a
vacuum tube. The electrical voltage causes one of the metal plates to become
positively charged (an anode) and one to become negatively charged (the
cathode, from which the device gets its name). Cathode ray tubes are the
basis of traditional television and computer monitor tubes.
When the electrical current was switched on, the tube would begin to glow
green. In 1897, Thomson was head of the Cavendish laboratory in Cambridge,
England, and set about to test the properties of this cathode ray tube glow.
He discovered that the glow was due to a beam of negatively charged particles
flying between the plates. These negatively charged particles later came to
be called electrons. Thomson also figured out that the electrons were
incredibly light — 2,000 times lighter than a hydrogen atom.
Thomson not only discovered the electron, but he theorized that the electron
was part of the atom (atoms weren't a completely accepted idea at the time)
that somehow got knocked free from the cathode and flowed through the
vacuum to the anode. With this discovery, scientists began discovering ways
to explore the inside of atoms.
Chapter 8: The Standard Model of Particle Physics / £j
The nucleus is the thinq in the middle
In the center of the atom is a dense ball of matter, called a nucleus, with a
positive electrical charge. Shortly after electrons were discovered, it became
clear that if you extracted an electron from an atom, the atom was left with
a slightly positive electrical charge. For a while, the assumption was that the
atom was a positively charged mass that contained negative electrons inside
of it, like pieces of negatively charged fruit in a positively charged fruitcake.
The entire fruitcake would be neutral unless you extracted some fruit from
it. (Scientists of the day, being of a different dietary constitution than most of
us today, explained it as plum pudding instead of fruitcake. Plum pudding or
fruitcake — it unappetizingly amounts to roughly the same picture.)
In 1909, however, an experiment by Hans Geiger and Ernest Marsden,
working under Ernest Rutherford, challenged this picture. These scientists
fired positively charged particles at a thin sheet of gold foil. Most of the
particles passed straight through the foil, but every once in a while one of
them bounced back sharply. Rutherford concluded that the positive charge
of the gold atom wasn't spread throughout the atom in the fruitcake model,
but was concentrated in a small positively charged nucleus, and that the rest
of the atom was empty space. The particles that bounced were the ones that
hit this nucleus.
Watching the dance inside an atom
In trying to figure out the atom's structure, a natural model for scientists to
look to was the planetary model, as shown in Figure 8-2. The electrons move
around the nucleus in orbits. Physicist Niels Bohr determined that these
orbits were governed by the same quantum rules that Max Planck had originally
applied in 1900 — that energy had to be transferred in discrete packets.
In astronomy, the Earth and sun are attracted to each other by gravity, but
because Earth is in motion around the sun, they never come into contact. A
similar model could explain why the negative and positive portions of the
atom never came into contact.
The first planetary model was proposed in 1904 by Nobel Prize-winner
Hantaro Nagaoka. It was based on the rings of Saturn and called the Saturnian
model. Certain details of the model were disproved by experiment, and
Nagaoka abandoned the model in 1908, but Ernest Rutherford revised the
concept to create his own planetary model in 1911, which was more consistent
with experimental evidence.
7 2i} Part " : The Ph y sics u P on Which String Theory Is Built _
When atoms emitted electrons, the electron's energy followed certain precise
patterns. Bohr realized in 1913 that this meant Rutherford's model required
some revision. To fit the patterns, he applied the idea that energy was
quantized, or bundled together in certain quantities, which allowed for stable
orbits (instead of the collapsing orbits predicted by electromagnetism). Each
electron could only exist in a certain, precisely defined energy state within its
orbit. To go from one orbit to a different orbit required the electron to have
enough energy to jump from one energy state to another.
Because of the quantum nature of the system, adding half the amount of
energy to go from one orbit to another didn't move the electron halfway
between those orbits. The electron remained in the first orbit until it received
enough energy to kick it all the way into the higher-energy state. This is yet
more of the strange behavior you've (hopefully) come to expect from quantum
physics.
The Rutherford-Bohr model works pretty well in describing the hydrogen
atom, but as atoms get more complex, the model begins to break down. Still,
the basic principles hold for all atoms:
j-" A nucleus is at the center of an atom.
w Electrons move in orbits around the nucleus.
w The electron orbits are quantized (they have discrete energy levels)
and are governed by the rules of quantum physics (though it would
take several years for those rules to become developed, as described in
Chapter 7).
.Chapter 8: The Standard Model of Particle Physics / 25
The Quantum Picture of the Photon:
Quantum Electrodynamics
The development of the theory of quantum electrodynamics (QED) was one of
the great intellectual achievements of the 20th century. Physicists were able
to redefine electromagnetism by using the new rules of quantum mechanics,
unifying quantum theory and electromagnetic theory. Quantum electrodynamics
was one of the first quantum approaches to a quantum field theory (described
in the next section), so it introduced many features possessed by string
theory (which is also a quantum field theory).
Quantum electrodynamics began with the attempt to describe particles
in terms of quantum fields, starting in the late 1920s. In the 1940s, QED
was completed three distinct times — by the Japanese physicist Sin-Itiro
Tomonaga during World War II and later by American physicists Richard
Feynman and Julian Schwinger. These three physicists shared the 1965 Nobel
Prize in Physics for this work.
Dr. Feynman's doodles explain how
particles exchange information
Though the principles of quantum electrodynamics were worked out by
three individuals, the most famous founder of QED was undeniably Richard
P. Feynman. Feynman was equally good at the mathematics and explanation
of a theory, which resulted in his creation of Feynman diagrams — a visual
representation of the mathematics that went on in QED.
Richard Phillips Feynman is one of the most interesting characters in 20th
century physics, easily ranking with Einstein in personality, if not in pure
fame. Early on in his career, Feynman made the conscious decision to only
work on problems that he found interesting, something that certainly served
him well. Fortunately for the world of physics, one of these problems was
quantum electrodynamics.
^jftBE/y Because electromagnetism is a field theory, the result of QED was a quantum
'y M\ field theory — a quantum theory that contains a value at every point in space.
iMJj ) You can imagine that the mathematics of such a theory was intimidating, to
say the least, even to those trained in physics and mathematics.
Feynman was brilliant not only with physical theory and mathematics,
but also with explanation. One way he simplified things was through the
application of his Feynman diagrams. Though the math was still complex,
126
Part II: The Physics Upon Which String Theory Is Built _
the diagrams meant you could begin talking about the physics without
needing all the complexity of the equations. And when you did need the
actual numbers, the diagrams helped organize your computations.
In Figure 8-3, you can see a Feynman diagram of two electrons approaching
each other. The Feynman diagram is set on a Minkowski space, as introduced
in Chapter 6, which depicts events in space-time. The electrons are the solid
lines (called propagators'), and as they get near to each other, a photon (the
squiggly propagator; see Chapter 7 for the basics of photons) is exchanged
between the two electrons.
Figure 8-3:
A Feynman
diagram
demon-
strates how
particles
interact with
each other.
In other words, in QED two particles communicate their electromagnetic
information by emitting and absorbing a photon. A photon that acts in this
manner is called a virtual photon or a messenger photon, because it's created
solely for the purpose of exchanging this information. This was the key insight
of QED, because without this exchange of a photon, there was no way to
explain how the information was communicated between the two electrons.
Also (and perhaps more important from a physics standpoint), a quantum field
theory (at least those that seem to match our real world) quickly reaches
infinity if distances become too small. To see how these infinities can arise,
consider both the fact that electromagnetic forces get larger at small distances
(infinitely larger at infinitely small distances) and also the distance and
momentum relationship from the uncertainty principle of quantum
mechanics (see Chapter 6 for details of the uncertainty principle). Even
talking about the instances where two electrons are incredibly close to each
other (such as within a Planck length) becomes effectively impossible in a
world governed by quantum physics.
.Chapter 8: The Standard Model of Particle Physics / 27
By quantizing electromagnetics, as QED does, Feynman, Schwinger, and
Tomonaga were able to use the theory despite these infinities. The infinities
were still present, but because the virtual photon meant that the electrons
didn't need to get so close to each other, there weren't as many infinities, and
the ones that were left didn't enter physical predictions. Feynman, Schwinger,
and Tomonaga took an infinite theory and extracted finite predictions. One of
the major motivations for the drive to develop a successful string theory is to
go even further and get an actually finite theory.
The mathematical process of removing infinities is called renormalization.
This is a set of mathematical techniques that can be applied to provide a
very carefully defined limit for the continuum of values contained in the field.
Instead of adding up all the infinite terms in the calculation and getting an
infinite result, physicists have found that applying renormalization allows
them to redefine parameters within the summation so it adds up to a finite
amount! Without introducing renormalization, the values become infinite, and
we certainly don't observe these infinities in nature. With renormalization,
however, physicists get unambiguous predictions that are among the most
precise and best-tested results in all of science.
Discovering that other kind
of matter: Antimatter
Along with the understanding of quantum electrodynamics, there came
a growing understanding that there existed antimatter, a different form
of matter that was identical to known matter, but with opposite charge.
Quantum field theory indicated that for each particle, there existed an
antiparticle. The antiparticle of the electron is called the positron.
In 1928, physicist Paul Dirac was creating the quantum theory of the electron
(a necessary precursor to a complete QED theory), when he realized that
the equation only worked if you allowed these extra particles — identical to
electrons but with opposite charge — to exist. Just four years later, the first
positrons were discovered and named by Carl D. Anderson while he was
analyzing cosmic rays.
The mathematics of the theory implied a symmetry between the known particles
and identical particles with opposite charge, a prediction that eventually
proved to be correct. The theory demanded that antimatter exist. String
theory implies another type of symmetry, called supersymmetry (see
Chapter 10), which has yet to be proved, but which many physicists believe
will eventually be discovered in nature.
/ 28 Part ll: The Physics Upon Which String Theory Is Built _
When antimatter comes in contact with ordinary matter, the two types of
matter annihilate each other in a burst of energy in the form of a photon.
This can also be depicted in QED with a Feynman diagram, as shown on the
left side of Figure 8-4. In this view, the positron is like an electron that moves
backward through time (as indicated by the direction of the arrow on the
propagator).
Figure 8-4:
(Left) A
particle and Time
antiparticle
annihilate
each other,
releasing
a photon.
(Right) A
photon
splits into
a particle
and antipar-
ticle, which
immediately
annihilate
each other.
Sometimes a particle is only Virtual
In quantum electrodynamics, virtual particles can exist briefly, arising from
the energy fluctuations of the quantum fields that exist at every point in
space. Some virtual particles — such as the photon in Figure 8-3 — exist just
long enough to communicate information about a force. Other virtual particles
spring into existence, seemingly for no purpose other than to make the lives
of physicists more interesting.
The existence of virtual particles is one of the strangest aspects of physics,
but it's a direct consequence of quantum physics. Virtual particles can exist
because the uncertainty principle, in essence, allows them to carry a large
fluctuation of energy, so long as they exist for only a brief period of time.
The right side of Figure 8-4 shows a pair of virtual particles — this time an
electron and a positron. In some cases, a photon can actually split into an
electron and positron and then recombine back into a photon.
.Chapter 8: The Standard Model of Particle Physics / 2y
The problem is that even though these particles are virtual, their effects have
to be taken into account when performing calculations about what takes
place in a given area. So no matter what you're doing, an infinite number of
strange virtual particles are springing into and out of existence all around
you, wreaking havoc with the smooth orderly calculations that you'd like
to perform! (If this sounds familiar, it's because this is the quantum foam
discussed in Chapter 2.)
biqqinq into the Nucleus:
Quantum Chromodynamics
As quantum physics attempted to expand into the nucleus of the atom, new
tactics were required. The quantum theory of the atomic nucleus, and the
particles that make it up, is called quantum chromodynamics (QCD). String
theory arose out of an attempt to explain this same behavior.
In the explanation of QED in the previous section, the only participants in
QED were the photon and the electron (and, briefly, the positron). In fact, QED
attempted to simplify the situation by only analyzing these two aspects of
the atom, which it could do by treating the nucleus as a giant, very distant
object. With QED finally in place, physicists were ready to take a good hard
look at the nucleus of the atom.
The pieces that make up
the nucleus: Nucteons
The nucleus of an atom is composed of particles called nucleons, which come
in two types: positively charged protons and the noncharged neutrons. The
protons were discovered in 1919, while the neutrons were discovered in 1932.
The proton is about 1,836 times as massive as the electron. The neutron is
about the same size as the proton, so the pair of them is substantially larger
than the electron. Despite this difference in size, the proton and electron
have identical electrical charges, but of opposite sign; the proton is positive
while the electron is negative.
The growth of technology allowed for the design and construction of larger
and more powerful particle accelerators, which physicists use to smash particles
into each other and see what comes out. With great delight, physicists began
smashing protons into each other, in the hopes of finding out what was
inside of them.
/ jf Part ll: The Physics Upon Which String Theory Is Built _
In fact, this work on trying to uncover the secrets of these nucleons would
lead directly to the first insights into string theory. A young physicist at
CERN applied an obscure mathematical formula to describe the behavior of
particles in a particle accelerator, and this is seen by many as the starting
point of string theory. (These events are covered in more detail in Chapter 10.)
The pieces that make up the
nucleoli's pieces: Quarks
Today, the nucleons are known to be types of hadrons, which are particles
made up of even smaller particles called quarks. The concept of quarks was
independently proposed by Murray Gell-Mann and George Zweig in 1964
(though the name, taken from James Joyce's Finnegan 's Wake, is pure Gell-
Mann), which in part earned Gell-Mann the 1969 Nobel Prize in Physics. The
quarks are held together by still other particles, called gluons.
In this model, both the proton and the neutron are composed of three
quarks. These quarks have quantum properties, such as mass, electrical
charge, and spin (see the next section for an explanation of spin). There
are actually a total of six flavors (or types) of quarks, all of which have been
experimentally observed:
v* Up quark
w Down quark
(-" Charm quark
i^ Strange quark
v" Top quark
v" Bottom quark
The properties of the proton and neutron are determined by the specific
combination of quarks that compose them. For example, a proton's charge
is reached by adding up the electrical charge of the three quarks inside it —
two up quarks and one down quark. In fact, every proton is made of two up
quarks and one down quark, so they're all exactly alike. Every neutron is
identical to every other neutron (composed of one up quark and two down
quarks).
In addition to standard quantum mechanical properties (charge, mass, and
spin), quarks have another property, which came out of the theory, called
color charge. This is somewhat similar to electrical charge in principle, but
it's an entirely distinct property of quarks. It comes in three varieties, named
.Chapter 8: The Standard Model of Particle Physics / jf /
red, green, and blue. (Quarks don't actually have these colors, because
they're much, much smaller than the wavelength of visible light. These are
just names to keep track of the types of charge.)
Because QED describes the quantum theory of the electrical charge, QCD
describes the quantum theory of the color charge. The color charge is the
source of the name quantum chromodynamics, because "chroma" is Greek
for "color."
In addition to the quarks, there exist particles called gluons. The gluons bind
the quarks together, kind of like rubber bands (in a very metaphoric sense).
These gluons are the gauge bosons for the strong nuclear force, just as the
photons are the gauge bosons for electromagnetism (see the later section on
gauge bosons for more on these particles).
Looking into the Types of Particles
Physicists have found a large number of particles, and one thing that proves
useful is that they can be broken down into categories based on their
properties. Physicists have found a lot of ways to do this, but in the following
sections I briefly discuss some of the most relevant categories to string
theory.
According to quantum mechanics, particles have a property known as spin.
This isn't an actual motion of the particle, but in a quantum mechanical
sense, it means that the particle always interacts with other particles as if it's
rotating in a certain way. In quantum physics, spin has a numerical value that
can be either an integer (0, 1, 2, and so on) or half-integer QA, %, and so on).
Particles that have an integer spin are called bosons, while particles that have
half-integer spin are called fermions.
Particles of force: Bosons
Bosons, named after Satyendra Nath Bose, are particles that have an integer
value of quantum spin. The bosons that are known act as carriers of forces in
quantum field theory, as the photon does in Figure 8-3. The Standard Model
of particle physics predicts five fundamental bosons, four of which have been
observed:
v* Photon
(^ Gluon (there are eight types of gluons)
/ 32 Part I': The Physics Upon Which String Theory Is Built _
v* Z boson
j-" W boson (actually two particles — the W + and W" bosons)
J-" Higgs boson (this one hasn't been found yet)
In addition, many physicists believe that there probably exists a boson called
the graviton, which is related to gravity. The relationship of these bosons to
the forces of physics are covered in the "Gauge Bosons: Particles Holding
Other Particles Together" section later in this chapter.
Composite bosons can also exist; these are formed by combining together an
even number of different fermions. For example, a carbon-12 atom contains
six protons and six neutrons, all of which are fermions. The nucleus of a
carbon-12 atom is, therefore, a composite boson. Mesons, on the other hand,
are particles made up of exactly two quarks, so they are also composite
bosons.
Particles of matter: Fermions
Fermions, named after Enrico Fermi, are particles that have a half-integer
value of quantum spin. Unlike bosons, they obey the Pauli exclusion principle,
which means that multiple fermions can't exist in the same quantum state.
While bosons are seen as mediating the forces of nature, fermions are par-
ticles that are a bit more "solid" and are what we tend to think of matter par-
ticles. Quarks are fermions.
In addition to quarks, there is a second family of fermions called leptons.
Leptons are elementary particles that can't (so far as scientists know) be
broken down into smaller particles. The electron is a lepton, but the Standard
Model of particle physics tells us that there are actually three generations
of particles, each heavier than the last. (The three generations of particles
were predicted by theoretical considerations before they were discovered by
experiment, an excellent example of how theory can precede experiment in
quantum field theory.)
Also within each generation of particles are two flavors of quarks. Table 8-1
shows the 12 types of fundamental fermions, all of which have been
observed. The numbers shown in Table 8-1 are the masses, in terms of
energy, for each of the known particles. (Neutrinos have virtually, but not
exactly, zero mass.)
Chapter 8: The Standard Model of Particle Physics / 33
Table 8-1
Elementary Particle Families for Fermions
Quarks
Leptons
First
Generation
Up Quark
3MeV
Down Quark
7MeV
Electron
Neutrino
Electron
0.5 MeV
Second
Generation
Charm
Quark
1.2 GeV
Strange Quark
120 MeV
Muon
Neutrino
Muon
106 MeV
Third
Generation
Top Quark
174 GeV
Bottom Quark
4.3 GeV
Tau
Neutrino
Tau
1.8 GeV
There are also, of course, composite fermions, made when an odd number
of fermions combine to create a new particle, such as how protons and
neutrons are formed by combining quarks.
Gauge Basons: Particles Holding
Other Panicles Together
In the Standard Model of particle physics, the forces can be explained in
terms of gauge theories, which possess certain mathematical properties.
These forces transmit their influence through particles called gauge bosons.
String theory allows gravity to be expressed in terms of a gauge theory,
which is one of its benefits. (One example of this is the AdS/CFT correspondence
discussed in Chapter 11.)
Throughout the development of the Standard Model, it became clear that all
the forces (or, as many physicists prefer, interactions') in physics could be
broken down into four basic types:
w Electromagnetism
Ie" Gravity
v" Weak nuclear force
V Strong nuclear force
The electromagnetic force and weak nuclear force were consolidated in the
1960s by Sheldon Lee Glashow, Abdus Salam, and Steven Weinberg into a
single force called the electroweak force. This force, in combination with
quantum chromodynamics (which defined the strong nuclear force), is what
physicists mean when they talk about the Standard Model of particle physics.
1 Sty Part " : The Ph V sics u P on Which String Theory Is Built _
One key element of the Standard Model of particle physics is that it's a gauge
theory, which means certain types of symmetries are inherent in the theory;
in other words, the dynamics of the system stay the same under certain
types of transformations. A force that operates through a gauge field is
transmitted with a gauge boson. The following gauge bosons have been
observed by scientists for three of the forces of nature:
(-" Electromagnetism — photon
IJ-" Strong nuclear force — gluon
u* Weak nuclear force — Z, W + , and W" bosons
In addition, gravity can be written as a gauge theory, which means that there
should exist a gauge boson that mediates gravity. The name for this theoretical
gauge boson is the graviton. (In Chapter 10, you see how the discovery of the
graviton in the equations of string theory led to its development as a theory of
quantum gravity.)
Exploring the Theory of Where
Mass Comes From
In the Standard Model of particle physics, particles get their mass through
something called the Higgs mechanism. The Higgs mechanism is based on
the existence of a Higgs field, which permeates all of space. The Higgs field
creates a type of particle called a Higgs boson. For the Higgs field to create
a Higgs boson takes a lot of energy, and physicists have so far been unable
to create one — so it's the only particle predicted by the Standard Model of
particle physics that hasn't been observed. This, together with attempts to
find new particles, such as those motivated by string theory, are among the
major reasons why scientists need advanced particle accelerators for more
high-energy experiments.
The weak nuclear force falls off very rapidly above short distances.
According to quantum field theory, this means that the particles mediating
the force — the W and Z bosons — must have a mass (as opposed to the
gluons and photons, which are massless).
The problem is that the gauge theories described in the preceding section
are mediated only by massless particles. If the gauge bosons have mass, then
a gauge theory can't be sensibly defined. The Higgs mechanism avoids this
problem by introducing a new field called the Higgs field. At high energies,
where the gauge theory is defined, the gauge bosons are massless, and the
theory works as anticipated. At low energies, the field triggers broken
symmetries that allow the particles to have mass.
.Chapter 8: The Standard Model of Particle Physics #3 J*
If the Higgs field does exist, it would create particles known as Higgs bosons.
The mass of the Higgs boson isn't something that the theory tells us, but
most physicists anticipate it to be found in the range of 150 GeV. Fortunately,
this is within the realm of what we can experimentally search for. Finding the
Higgs boson would be the final confirmation of the Standard Model of particle
physics.
The Higgs mechanism, Higgs field, and Higgs boson are named after Scottish
physicist Peter Higgs. Though he wasn't the first to propose these concepts,
he's the one they were named after, which is just one of those things that
sometimes happens in physics.
For a discussion on the Higgs mechanism in depth, I recommend Lisa
Randall's Warped Passages: Unraveling the Mysteries of the Universe's Hidden
Dimensions. Chapter 10 of that book is devoted entirely to this topic. You
could also look to The God Particle: If the Answer is the Universe, What is
the Question? by Nobel Laureate Leon Lederman and Dick Teresi, which is
devoted entirely to the topic of the search for the Higgs boson.
From Big to Small: The Hierarchy
Problem in Physics
The Standard Model of particle physics is an astounding success, but it
hasn't answered every question that physics hands to it. One of the major
questions that remains is the hierarchy problem, which seeks an explanation
for the diverse values that the Standard Model lets physicists work with.
Many physicists feel that string theory will ultimately be successful at
resolving the hierarchy problem.
For example, if you count the theoretical Higgs boson (and both types of W
bosons), the Standard Model of particle physics has 18 elementary particles.
The masses of these particles aren't predicted by the Standard Model.
Physicists had to find these by experiment and plug them into the equations
to get everything to work out right.
If you look back at Table 8-1, you notice three families of particles among the
fermions, which seems like a lot of unnecessary duplication. If we already
have an electron, why does nature need to have a muon that's 200 times as
heavy? Why do we have so many types of quarks?
Beyond that, when you look at the energy scales associated with the quantum
field theories of the Standard Model, as shown in Figure 8-5, even more
questions may occur to you. Why is there a gap of 16 orders of magnitude (16
zeroes!) between the intensity of the Planck scale energy and the weak scale?
/ 3 Part " : The Physics Upon Which String Theory Is Built _
Energy Length
KPGeV-
-•-Planck scaler-
-10- 33 cm
10 ,8 GeV-
t .
10 ,5 GeV-
-10- 30 cm
10 ,2 GeV-
E
-10- 27 cm
Figure 8-5:
The hierar-
chy problem
in physics
10 9 GeV-
10 6 GeV-
1
-10- 24 cm
-10r 21 cm
relates
'-«- weak scaler
-I0" 18 cm
to the
large gap
10 3 GeV-
(TeV)
-I0" 15 cm
between the
GeV
-•-proton mass-*-
weak scale
-10 ,2 cm
and Planck
scale of
length and
energy.
10 3 GeV-
(MeV)
10 6 GeV-
(keV)
-•-electron mass*-
-10~ 9 cm
At the bottom of this scale is the vacuum energy, which is the energy generated
by all the strange quantum behavior in empty space — virtual particles
exploding into existence and quantum fields fluctuating wildly due to the
uncertainty principle.
The hierarchy problem occurs because the fundamental parameters of the
Standard Model don't reveal anything about these scales of energy. Just as
physicists have to put the particles and their masses into the theory by hand,
so too have they had to construct the energy scales by hand. Fundamental
principles of physics don't tell scientists how to transition smoothly from
talking about the weak scale to talking about the Planck scale.
As I explain in Chapter 2, trying to understand the "gap" between the weak
scale and the Planck scale is one of the major motivating factors behind
trying to search for a quantum gravity theory in general, and string theory in
particular. Many physicists would like a single theory that could be applied
at all scales, without the need for renormalization (the mathematical process
of removing infinities), or at least to understand what properties of nature
determine the rules that work for different scales. Others are perfectly happy
with renormalization, which has been a major tool of physics for nearly 40
years and works in virtually every problem that physicists run into.
Chapter 9
Physics in Space: Considering
Cosmology and Astrophysics
In This Chapter
Putting things where they belong in the universe
Going back to the universe's teeny-tiny beginnings
Getting enlightened about dark matter and dark energy
Seeing how black holes bend and break space
■ Mne of mankind's first scientific acts was probably to look into the
\r heavens and ask questions about the nature of that expansive universe.
Today, scientists are still fascinated by these questions, and with good
reason. Though we know much more than our cave-dwelling ancestors did
about what makes up the heavens, the black space between the stars still
holds many mysteries — and string theory is at the heart of the search for
the answers to many of these mysteries.
In this chapter, you find out what physicists, astronomers, astrophysicists,
and cosmologists have uncovered about the workings of the universe
independent of string theory. As these scientists have discovered how the
universe works, their findings have led to more difficult questions, which
string theorists hope to answer. I cover some of these more complex points
about the universe in Chapter 14. This chapter gives you the background
that will help you understand the ties between cosmology, astrophysics, and
string theory.
In the following pages, I explore the consequences of Einstein's relativity,
where scientists find that the universe seems to have had a beginning. At
this point, scientists were able to determine where the particles in our
universe come from. The theory of the universe's origin grows more complex
with the introduction of a rapidly expanding early universe. I also introduce
you to two of cosmology's biggest mysteries: the presence of unseen dark
matter and of repulsive gravity in the form of dark energy. Finally, I provide
a glimpse into black holes, objects that later become important to string
theory.
/3o Part " : The Physics Upon Which String Theory Is Built
Creating an Incorrect Model
of the Universe
Before string theory, there was Einstein's relativity, and before that was
Newton's gravity, and for about two centuries before Newton, the laws
governing the universe were believed, by most of the Western world, to be
those set out by Aristotle. Understanding the later revolutions in cosmology
starts with the original models of the universe developed by the ancient Greeks.
Aristotle assigns realms to the universe
Aristotle pictured a universe that was made of a substance called the aether
(see Chapter 5 for more about this elusive element). The heavens, to him and
his followers, were a place of unsurpassed geometric elegance and beauty
that didn't change over time.
In some ways, Aristotle is seen as one of the first scientists. He spent a great
deal of time discussing the importance of observation to understand nature.
Aristotle described the universe as containing five fundamental elements:
earth, air, fire, water, and aether. The heavens were the realm of aether, but
we were stuck down with the earth, air, fire, and water.
Aristotle knew Earth was a sphere, and he thought that each element had a
natural location within that sphere, as shown in Figure 9-1. The natural
location of the earth element was at the center of the sphere — this was
considered the earth realm. Next came the water realm, followed by the air,
fire, and finally aether realms. (The moon resided somewhere on the border
of the aether realm, probably right on the edge of the fire realm.)
The clouds — composed of air and water elements — drifted in the air, along
the border of the air and water realms. You can mix water and earth to make
mud, but the earth part tends to eventually settle on the bottom because the
earth realm is beneath the water realm. When a fire was ignited, the flames
reached up into the sky in an effort to reach the fire realm, where the sun
resided.
In Aristotle's model, the outermost sphere was the aether realm, relatively
untouched by the mundane elements, aside from the moon (hardly mundane)
and its border with the fire realm. It was a perfect realm, which contained the
stars, fixed in place on a serene, eternal background. This belief defined the
heavens for well over a thousand years.
_ Chapter 9: Physics in Space: Considering Cosmology and Astrophysics / jy
Ptolemy puts Earth at the center of the
universe {and the Catholic Church agrees)
The cosmological model of the stars' movements built on Aristotle's
philosophy was called the Ptolemaic model, after the man who invented it.
Ptolemy lived in Roman Egypt during the second century AD, doing his
principle work in the city of Alexandria. His book on astronomy, the Almagest
(which roughly translates to "the greatest") was written in approximately 150
AD. The greatest achievement of this volume was to attempt to describe the
motion of the heavens in precise mathematical language.
The model described by Ptolemy, and maintained by most scholars until the
time of Copernicus and Galileo, was a geosynchronous model of the heavens,
in which Earth was at the center of the universe. The reason for such a model
is obvious from Aristotle's elemental spheres depicted in Figure 9-1: Earth
has a distinct, unique place in the universe.
In Ptolemy's geosynchronous model, the moon, planets, and sun are
mounted on rotating spheres around Earth. Beyond the planets is the largest
sphere, which has the stars mounted on it. This model accurately predicted
the motion of the planets, so it was well received.
The Catholic Church adopted this model of the universe for a number of
reasons. One is that it provided a way for the sun to be "held still" in the sky
to match a Biblical account. Another reason is that the theory said nothing
about what was outside the star-laden spheres, so it left plenty of room for
heaven and hell.
/ 1} Part ll: The Physics Upon Which String Theory Is Built _
So many scientists, so many names
The names for different types of space
scientists can get rather confusing. Gone are
the days when anyone who looked through
a telescope could be called an astronomer.
The distinction between astronomer and
astrophysicist is pretty much history, and the
line between astrophysicist and cosmologist
gets blurry in the realm of string theory. The
term used is often chosen out of personal
preference, but there are some guidelines:
e* Astronomer: This is the classical term
for a scientist who studies the heavens.
Since Galileo, optical telescopes have
been the primary tool used to examine
celestial bodies. Today, the telescopes can
be radio, x-ray, or gamma ray telescopes,
which see light in the nonvisual spectrum.
Traditionally, astronomers have devoted
more time to classification and description
of bodies in space than to attempting to
explain the phenomena.
i^ Astrologer: In the time of Ptolemy through
Copernicus, the terms astrologer and
astronomer were essentially synonyms.
Since Copernicus, they have become more
distinct; today they represent radically
different disciplines, with astrology well
outside the bounds of science. An astrologer
tries to find a connection between human
behaviors and the motion of celestial
bodies, generally with a vague or
supernatural mechanism introduced as the
basis for these connections. See Astrology
For Dummies, 2nd Edition, by Rea Orion
(Wiley) for more information on the field.
(^ Astrophysicist: This term applies to
someone who studies the physics of
interactions within and between stellar
bodies. Astrophysicists seek to apply the
principles of physics to create general
laws governing the behavior of these
interactions.
i^ Cosmologist: This term is used for a type of
astrophysicist who focuses on the evolution
of the universe — the processes of how the
universe changes over time. A cosmologist
rarely cares about a specific stellar body or
solar system, and galaxies are frequently
too parochial for these explorers of space.
Cosmologists often focus their attention on
theories that use unimaginably large scales
of time, space, and energy. The study of
the big bang, or the universe's end, is an
example of the cosmologist's domain.
Perhaps most significantly, the Church embraced the belief that Earth and
the heavens were made of different things. Our realm was special. In all of
space there was nothing else quite like Earth, and certainly no other place
that could give rise to anything resembling humanity. With the Catholic
Church's official endorsement, the Ptolemaic model of the universe became
not just a scientific theory, but a religious fact.
Chapter 9: Physics in Space: Considering Cosmology and Astrophysics / [l /
The Enlightened Universe:
Some Changes AiioWed
In the 1500s, the geosynchronous model was replaced with the heliocentric
model, in which the sun was at the center of the solar system. (Heliocentric
models had originally been proposed by Greeks such as Aristarchus,
but Aristotle's model gained greater popularity.) The work of Nicholas
Copernicus and Galileo Galilei was key to this revolution, which dislodged us
from our special place at the center of the universe. The result has become
known as the Copernican principle, which says that space looks the same no
matter where you view it from.
Copernicus corrects What's
Where in the universe
The Ptolemaic model was based on the idea that all the celestial objects —
planets, moons, stars, and so on — were on concentric spheres, each of
which was centered on Earth. Over the centuries (from about 150 BC to 1500
AD), though, observations made it clear that this wasn't the case.
To preserve the Ptolemaic model, it was modified over the years. Celestial
objects were mounted on spheres that were then mounted on other spheres.
The very elegance that made the Ptolemaic model so appealing was gone,
replaced with a mishmash of geometric nonsense that only partially
conformed with scientific observations — which were growing more and
more precise due to new technologies.
This was the prime time for a scientific revolution. The existing theory was
failing, but without another system in place to adopt (the heliocentric models
of Aristarchus were ignored, for some reason), the prevailing system continued
to be modified in increasingly improbable ways (check out Chapter 4 for
more on this process). In the case of the Ptolemaic model, the fact that
contradicting it was heretical didn't help incite a scientific revolution either.
In his book, On the Revolutions of the Celestial Spheres, the Polish astronomer
Nicholas Copernicus explained his heliocentric model, making it clear that
the sun, not Earth, sat at center stage. He still used spheres, though, and
made other assumptions that haven't born the test of time, but it was a major
improvement over the Ptolemaic model.
/ If 2 Part I': The Physics Upon Which String Theory Is Built _
Copernicus published his heliocentric model upon his death in 1543, fearing
retribution from the Church if he published it earlier (although he did hand
out versions of the theory to friends about 30 years earlier). Some Indian
writers made this heliocentric claim as far back as the seventh century AD,
and some Islamic astronomers and mathematicians studied this idea as well,
but it's unclear to what degree Copernicus was aware of their work.
Copernicus was a theorist, not an observational astronomer. His key insight
was the idea that Earth didn't have a distinct position within the universe, a
concept that was named the Copernican principle in the mid-20th century.
Beholding the movements
of heavenly bodies
One of the greatest observational astronomers of this revolutionary age
was Tycho Brahe, a Danish nobleman who lived from 1546 to 1601. Brahe
made an astounding number of detailed astronomical observations. He used
his family's wealth to found an observatory that corrected nearly every
astronomical record of the time, including those in Ptolemy's Almagest.
Using Brahe's measurements, his assistant Johannes Kepler was able to
create rules governing the motion of the planets in our solar system. In his
three laws of planetary motion, Kepler realized that the planetary orbits were
elliptical rather than circular.
More importantly, Kepler discovered that the motion of the planets wasn't
uniform. A planet's speed changes as it moves along its elliptical path. Kepler
showed that the heavens were a dynamic system, a detail that later helped
Newton show that the sun constantly influences the planets' motion.
Galileo, by using the telescope, later realized that other planets had moons
and determined that the heavens weren't static. The Catholic Church
charged him with heresy. To get away with only house arrest, Galileo was
forced to recant his observations about the movements of heavenly bodies.
Reportedly, his final words on his death bed were, "But they do move!" (Some
versions of this story indicate that he uttered this statement upon being
sentenced, so it may be a myth.)
Galileo's work, together with Kepler's, laid the foundation for Isaac Newton's
law of gravity. With gravity introduced, the final nail had been placed in the
scientific consensus behind the geosynchronous view. Astronomers and
physicists now knew that Earth circled the sun, as the heliocentric model
described. (The Catholic Church officially endorsed the heliocentric view in
the 19th century. In 1992, Pope John Paul II officially apologized for Galileo's
treatment.)
Chapter 9: Physics in Space: Considering Cosmology and Astrophysics / uj
Introducing the Idea of
an Expanding Universe
Even two centuries after Newton, Albert Einstein was strongly influenced
by the concept of an unchanging universe. His general theory of relativity
predicted a dynamic universe — one that changed substantially over time —
so he introduced a term, called the cosmological constant, into the theory to
make the universe static and eternal. This would prove to be a mistake when,
several years later, astronomer Edwin Hubble discovered that the universe
was expanding! Even today, the consequence of the cosmological constant
in general relativity has enormous impact upon physics, causing string
theorists to rethink their whole approach.
The equations of general relativity that Einstein developed showed that the
very fabric of space was expanding or contracting. This made no sense to
Einstein, so in 1917 he added the cosmological constant to the equations.
This term represented a form of repulsive gravity that exactly balanced out
the attractive pull of gravity.
When Hubble showed that the universe was indeed expanding, Einstein
called the introduction of the cosmological constant his "biggest blunder"
and removed it from the equations. This concept would return over the
years, however, as you see in the "Dark Energy: Pushing the Universe Apart"
section later in this chapter. With the discovery of dark energy, Einstein's
"blunder" was found to be a necessary parameter in the theory (even though
physicists for most of a century assumed the cosmological constant's value
was zero).
Discovering that energy and
pressure hatie gravity
In Newton's gravity, bodies with mass were attracted to each other.
Einstein's relativity showed that mass and energy were related. Therefore,
mass and energy both exerted gravitational influence. Not only that, but
it was possible that space itself could exert a pressure that warped space.
Several models were constructed to show how this energy and pressure
affected the expansion and contraction of space.
When Einstein created his first model based on the general theory of
relativity, he realized that it implied an expanding universe. At the time,
no one had any particular reason to think the universe was expanding, and
Einstein assumed that this was a flaw in his theory.
/ l) 1} Part II: The Physics Upon Which String Theory Is Built _
Einstein's general relativity equations allowed for the addition of an extra
term while remaining mathematically viable. Einstein found that this term
could represent a positive energy (or negative pressure) uniformly distributed
throughout the fabric of space-time itself, which would act as an antigravity,
or repulsive form of gravity. This term was chosen to precisely cancel out the
contraction of the universe, so the universe would be static (or unchanging
in time).
In 1917, the same year Einstein published his equations containing the
cosmological constant, Dutch physicist Willem de Sitter applied them to a
universe without matter. (As I explain in Chapter 4, this is a frequent step in
scientific analysis — you strip a scientific theory of all the complications and
consider it in the simplest cases.)
In this de Sitter space, the only thing that exists is the energy of the vacuum —
the cosmological constant itself. Even in a universe containing no matter at all,
this means that space will expand. A de Sitter space has a positive value for
the cosmological constant, which can also be described as a positive curvature
of space-time. A similar model with a negative cosmological constant (or a
negative curvature, in which expansion is slowing) is called an anti-de Sitter
space. (More on the curvature of space-time in a bit.)
In 1922, the Russian physicist Aleksandr Friedmann turned his hand to
solving the elaborate equations of general relativity, but decided to do so in
the most general case by applying the cosmological principle (which can be
seen as a more general case of the Copernican principle), which consists of
two assumptions:
IV The universe looks the same in all directions (it's isotropic).
e* The universe is uniform no matter where you go (it's homogenous).
With these assumptions, the equations become much simpler. Einstein's
original model and de Sitter's model both ended up being special cases
of this more general analysis. Friedmann was able to define the solution
depending on just three parameters:
Ii^ Hubble's constant (the rate of expansion of the universe)
u* Lambda (the cosmological constant)
v" Omega (average matter density in the universe)
To this day, scientists are trying to determine these values as precisely as
they can, but even without real values they can define three possible solutions.
Each solution matches a certain "geometry" of space, which can be represented
in a simplified way by the way space naturally curves in the universe, as
shown in Figure 9-2.
_ Chapter 9: Physics in Space: Considering Cosmology and Astrophysics / [l J
v* Closed universe: There is enough matter in the universe that gravity
will eventually overcome the expansion of space. The geometry of such
a universe is a positive curvature, such as the sphere in the leftmost
image in Figure 9-2. (This matched Einstein's original model without a
cosmological constant.)
(-" Open universe: There isn't enough matter to stop expansion, so the
universe will continue to expand forever at the same rate. This space-
time has a negative curvature, like the saddle shape shown in the middle
image in Figure 9-2.
J-" Flat universe: The expansion of the universe and the density of matter
perfectly balance out, so the universe's expansion slows down over time
but never quite stops completely. This space has no overall curvature,
as shown in the rightmost image of Figure 9-2. (Friedmann himself didn't
discover this solution; it was found years later.)
These models are highly simplified, but they needed to be because Einstein's
equations got very complex in cases where the universe was populated with
a lot of matter, and supercomputers didn't yet exist to perform all the math
(and even physicists want to go on dates every once in a while).
Hubbte drives it home
In 1927, astronomer Edwin Hubble proved that the universe is expanding.
With this new evidence, Einstein removed the cosmological constant from his
equations.
Edwin Hubble had shown in 1925 that there were galaxies outside our own.
Until that time, astronomers had observed white blobs of stars in the sky,
which they called nebulae, but the astronomers disagreed about how far
away they were. In his work at the Mount Wilson Observatory in California,
Hubble proved that these were, in fact, distant galaxies.
/ 1} Part " : The Physics Upon Which String Theory Is Built _
While studying these distant galaxies, he noticed that the light from these
distant stars had a wavelength that was shifted slightly toward the red end of
the electromagnetic spectrum, compared to what he expected.
This is a consequence of the wave nature of light — an object that's moving
(with respect to the observer) emits light with a slightly different wavelength.
This is based on the Doppler effect, which is what happens to the wavelength
of sound waves from a moving source. If you've ever heard a siren's pitch
change as it approaches and passes you, you've experienced the Doppler
effect.
In a similar way, when a light source is moving, the wavelength of the light
changes. A redshift in light from a star means the star is moving away from
the observer.
Hubble saw this redshift in the stars he observed, caused not only by the
motion of the stars but by the expansion of space-time itself, and in 1929
determined that the amount of shift was related to the distance from Earth.
The more distant stars were moving away faster than the nearby stars. Space
itself was expanding.
Clearly, in this case, Einstein had been wrong and Friedmann had been
right to explore all the possible scenarios predicted by general relativity.
(Unfortunately, Friedmann died in 1925, so he never knew he was right.)
Finding a Beginning:
The Big Bang Theory
It soon became evident that an expanding universe was once very much
smaller — so small, in fact, that it was compressed down to a single point (or,
at least, a very small area). The theory that the universe started from such
a primordial point and has expanded ever since is known as the big bang
theory. The theory was first proposed in 1927, but was controversial until
1965, when an accidental discovery supported the theory. Today, the most
advanced astronomical observations show that the big bang theory is likely
true. String theory will hopefully help physicists understand more precisely
what happened in those early moments of the universe, so understanding the
big bang theory is a key component of string theory's cosmological work.
The man originally responsible for the big bang theory was a Belgian priest
and physicist, Georges LemaTtre, who independently worked on theories
similar to Friedmann's. Like Friedmann, LemaTtre realized that the universe
defined by general relativity would either expand or contract.
_ Chapter 9: Physics in Space: Considering Cosmology and Astrophysics / (l(
What's in a name?
The name "big bang" was given to the theory
by Fred Hoyle, one of the theory's greatest
critics. In a 1949 series of BBC radio broadcasts,
Hoyle was speaking dismissively of the idea
that everything in the universe was created in
one sudden "big bang" in the distant past.
The name stuck, much to big bang theorists'
dismay. Strictly speaking, the big bang theory
doesn't include a bang. Rather, the theory
states that a tiny primordial particle began to
expand, creating the universe. There is neither
big nor bang in this theory.
In 1927, LemaTtre learned of Hubble's finding about distant galaxies moving
away from Earth. He realized that this meant space was expanding, and
he published a theory that came to be called the big bang theory. (See the
nearby sidebar, "What's in a name?")
Because you know that space is expanding, you can run the video of the
universe backward in time in your head (rewind it, so to speak). When you do
this, you realize that the universe had to be much smaller than it is now. As
the matter in the universe gets compressed into a smaller and smaller amount
of space, the laws of thermodynamics (which govern the flow of heat) tell you
that the matter had to be incredibly hot and dense.
The big bang theory reveals that the universe came from a state of dense,
hot matter, but it tells nothing about how the matter got there, or whether
anything else existed before the big bang (or even if the word "before" has
any meaning when you're talking about the beginning of time). I explore these
speculative topics in Chapters 14 and 15.
Bucking the bla bana:
The steady state theory
In opposition to the big bang theory, Fred Hoyle proposed an alternative
theory, called the steady state theory. In this theory, new particles were
continually being created. As space expanded, these new particles were
created fast enough that the overall mass density of the universe remained
constant.
To understand the reason for such a theory, you have to realize that few
physicists thought it likely that a dense ball of matter could spring into
existence out of nowhere, violating the law of conservation of mass (or
conservation of mass-energy). That matter had to come from somewhere.
1 1)8 Part H: The Physics Upon Which String Theory Is Built _
In Hoyle's view, if matter could be created out of nothing one time, then why
not have it happen all the time?
Though Hoyle's steady state theory would ultimately fail, in trying to prove
it Hoyle would prove himself worthy in the eyes of history by developing
a theory about where the dense atoms of our universe come from (which I
cover in the later section "Understanding where the chemical elements came
from").
Going to bat for the big bang: Cosmic
microWaOe background radiation
One of the major converts to the big bang theory was physicist George
Gamow, who realized that if the theory were true, a residual trace of cosmic
microwave background radiation (CMBR) would be spread throughout the
universe. Attempts to find this radiation failed for many years, until an
unexpected problem in 1965 accidentally detected it.
Gamow is known to many as the author of a number of popular books on
science, but he was also a theoretician and experimentalist who liked to
throw out ideas right and left, seemingly not caring whether they bore fruit.
Turning his attention to cosmology and the big bang, Gamow noted in 1948
that this dense ball of matter (probably neutrons, he hypothesized) would
emit black body radiation, which had been worked out in 1900 by Max
Planck. A black body emits radiation at a definable wavelength based on the
temperature.
Gamow's two students, Ralph Alpher and Robert Herman, published a paper
in 1948 with the calculation for the temperature, and therefore the radiation, of
this original ball of matter. The men calculated the temperature to be about
5 degrees above absolute zero, although it took nearly a year for Gamow to
agree with this calculation. This radiation is in the microwave range of the
electromagnetic spectrum, so it's called the cosmic microwave background
radiation (CMBR).
Although this was a successful theoretical breakthrough, it went largely
unnoticed at the time. Nobody conducted a serious experiment to look for
this radiation, even while Gamow, Alpher, and Herman tried to gain support.
In 1965, a Princeton University team led by Robert Dicke had independently
developed the theory and was attempting to test it. Dicke's team failed to
discover the CMBR, however, because while they were putting the finishing
touches on their equipment, someone else beat them to it.
_ Chapter 9: Physics in Space: Considering Cosmology and Astrophysics 1 Uy
A few miles away, at New Jersey's Bell Laboratory Holmdell Horn Radio
Telescope, Arno Penzias and Robert Wilson were having trouble of their
own. Their telescope — which was more sophisticated than Princeton
University's — was picking up this horrible static when they attempted to
detect radio signals in space. No matter where they pointed the silly thing,
they kept getting the same static. The two men even cleaned bird droppings
off the telescope, but to no avail. In fact, the static got worse on the
unobstructed telescope.
Fortunately, Penzias and Dicke had a mutual friend in astronomer Bernard
Burke, and upon discovering the problems the two men had, he introduced
them. Penzias and Wilson earned the 1978 Nobel Prize in Physics for
accidentally discovering the CMBR (at a temperature of 2.7 degrees above
absolute zero — Gamow's calculations had been slightly high).
Forty more years of research has only confirmed the big bang theory, most
recently in the picture of the CMBR obtained by the Wilkinson Microwave
Anisotropy Probe (WMAP) satellite. The picture obtained by this satellite,
shown in Figure 9-3, is like a baby picture of the universe when it was just
380,000 years old (13.7 billion years ago). Before this, the universe was dense
enough to be opaque, so no light can be used to look further back than that.
Courtesy of NASA
For more information on the WMAP satellite, check out the official WMAP Web
site at NASA's Goddard Space Flight Center, map . gsf c . nasa . gov.
/ 50 Part " : The Physics Upon Which String Theory Is Built
Understanding where the chemical
elements came from
Both George Gamow and Fred Hoyle, while differing strongly on the big
bang theory, were the key figures in determining the process of stellar
nucleosynthesis, in which atoms are made inside of stars. Gamow theorized
that elements were created by the heat of the big bang. Hoyle showed that
the heavier elements were actually created by the intense heat of stars and
supernovas.
Gamow's original theory was that as the intense heat of the expanding
universe cooled, the lightest element, hydrogen, was formed. The energy at
this time was still enough to cause hydrogen molecules to interact, perhaps
fusing into helium atoms. Estimates show that nearly 75 percent of the
visible universe is made up of hydrogen and 25 percent is helium, with the
rest of the elements on the periodic table making up only trace amounts on
the scale of the entire universe.
This proved to be good, because Gamow couldn't figure out how to cook up
many of those heavier elements in the big bang. Hoyle tackled the problem,
assuming that if he could make all the elements in stars, then the big bang
theory would fail. Hoyle's work on stellar nucleosynthesis was published in
1957.
In Hoyle's nucleosynthesis method, helium and hydrogen gather inside of
stars and undergo nuclear fusion. Even this, however, isn't hot enough to
make atoms more massive than iron. These heavier elements — zinc, copper,
uranium, and many others — are created when massive stars go through
their deaths and explode in giant supernovas. These supernovas produce
enough energy to fuse the protons together into the heavy atomic nucleus.
The elements are then blown out into space by the supernova blast, drifting
as clouds of stellar dust. Some of this stellar dust eventually falls together
under the influence of gravity to form planets, such as our Earth.
Using Inflation to Sot</e the Universe's
Problems of Flatness and Horizon
In trying to understand the universe, two major problems remained: the
flatness problem and the horizon problem. To solve these two problems, the
big bang theory is modified by the inflation theory, which states that the
universe expanded rapidly shortly after it was created. Today, the principles
at the heart of inflation theory have a profound impact on the way that string
theory is viewed by many physicists, as becomes clear in Chapter 14.
_ Chapter 9: Physics in Space: Considering Cosmology and Astrophysics j f) /
These two problems can be stated simply a
u Horizon problem: The CMBR is essentially the same temperature in a
directions.
j-" Flatness problem: The universe appears to have a flat geometry.
The universe's issues: Too far and too flat
The horizon problem (also sometimes called the homogeneity problem) is
that no matter which direction you look in the universe, you see basically the
same thing (see Figure 9-3). The CMBR temperatures throughout the universe
are, to a very high level of measurement, almost exactly the same temperature
in every direction. This really shouldn't be the case, if you think about it
more carefully.
If you look in one direction in space, you're actually looking back in time.
The light that hits your eye (or telescope) travels at the speed of light, so it
was emitted years ago. This means there's a boundary of 14 billion (or so)
light-years in all directions. (The boundary is actually farther because space
itself is expanding, but you can ignore that for the purposes of this example.)
If there is anything farther away than that, there is no way for it to have ever
communicated with us. So you look out with your powerful telescope and can
see the CMBR from 14 billion light-years away (call this Point A).
If you now look 14 billion light-years in the opposite direction (call this Point
B), you see exactly the same sort of CMBR in that direction. Normally, you'd
take this to mean that all the CMBR in the universe has somehow diffused
throughout the universe, like heating up an oven. Somehow, the thermal
information is communicated between Points A and B.
But Points A and B are 28 billion light-years apart, which means, because no
signal can go faster than the speed of light, there's no way they could have
communicated with each other in the entire age of the universe. How did they
become the same temperature if there's no way for heat to transfer between
them? This is the horizon problem.
The flatness problem has to do with the geometry of our universe, which
appears (especially with recent WMAP evidence) to be a flat geometry, as
pictured in Figure 9-2. The matter density and expansion rate of the universe
appear to be nearly perfectly balanced, even 14 billion years later when
minor variations should have grown drastically. Because this hasn't happened,
physicists need an explanation for why the minor variations haven't
increased dramatically. Did the variations not exist? Did they not grow into
large-scale variations? Did something happen to smooth them out? The
flatness problem seeks a reason why the universe has such a seemingly
perfectly flat geometry.
/ §2 Part ll: The Physics Upon Which String Theory Is Built
Rapid expansion early on
holds the solutions
In 1980, astrophysicist Alan Guth proposed the inflation theory to solve
the horizon and flatness problems (although later refinements by Andrei
Linde, Andreas Albrecht, Paul Steinhardt, and others were required to get it
to work). In this model, the early universal expansion accelerated at a rate
much faster than we see today.
It turns out that the inflationary theory solves both the flatness problem
and horizon problem (at least to the satisfaction of most cosmologists and
astrophysicists). The horizon problem is solved because the different regions
we see used to be close enough to communicate, but during inflation, space
expanded so rapidly that these close regions were spread out to cover all of
the visible universe.
The flatness problem is resolved because the act of inflation actually flattens
the universe. Picture an uninflated balloon, which can have all kinds of
wrinkles and other abnormalities. As the balloon expands, though, the surface
smoothes out. According to inflation theory, this happens to the fabric of the
universe as well.
In addition to solving the horizon and flatness problems, inflation also
provides the seeds for the structure that we see in our universe today.
Tiny energy variations during inflation, due simply to quantum uncertainty,
become the sources for matter to clump together, eventually becoming
galaxies and clusters of galaxies.
One issue with the inflationary theory is that the exact mechanism that
would cause — and then turn off — the inflationary period isn't known.
Many technical aspects of inflationary theory remain unanswered, though
the models include a scalar field called an inflaton field and a corresponding
theoretical particle called an inflaton. Most cosmologists today believe that
some form of inflation likely took place in the early universe.
Some variations and alternatives to this model are posed by string theorists
and other physicists. Two creators of inflation theory, Andreas Albrecht and
Paul J. Steinhart, have worked on alternative theories as well; see Chapter 14
for Steinhart's ekpyrotic theory and Chapter 19 for Albrecht's variable speed
of light cosmology.
Chapter 9: Physics in Space: Considering Cosmology and Astrophysics 133
Dark Matter: The Source of Extra Gravity
Astronomers have discovered that the gravitational effects observed in
our universe don't match the amount of matter seen. To account for these
differences, it appears that the universe contains a mysterious form of matter
that we can't observe, called dark matter. Throughout the universe, there's
approximately six times as much dark matter as normal visible matter — and
string theory may explain where it comes from!
In the 1930s, Swiss astronomer Fritz Zwicky first observed that some galaxies
were spinning so fast that the stars in them should fly away from each other.
Unfortunately, Zwicky had personality clashes with many in the astronomy
community, so his views weren't taken very seriously.
In 1962, astronomer Vera Rubin made the same discoveries and had nearly
the same outcome. Though Rubin didn't have the same issues of temperament
that Zwicky did, many disregarded her work because she was a woman.
Rubin maintained her focus on the problem and, by 1978, had studied 11
spiral galaxies, all of which (including our own Milky Way) were spinning so
fast that the laws of physics said they should fly apart. Together with work
from others, this was enough to convince the astronomy community that
something strange was happening.
Whatever is holding these galaxies together, observations now indicate that
there has to be far more of it than there is the visible matter that makes up
the baryonic matter that we're used to — the matter that comprises you, this
book, this planet, and the stars.
Physicists have made several suggestions about what could make up this
dark matter, but so far no one knows for sure. String theorists have some
ideas, which you can read about in Chapter 14.
bark Energy: Pushing the Universe Apart
Einstein's cosmological constant allowed for a uniform repulsive energy
throughout the universe. Since Hubble discovered the expansion of the
universe, most scientists have believed that the cosmological constant was
/ ylf Part II: The Physics Upon Which String Theory Is Built _
zero (or possibly slightly negative). Recent findings have indicated that the
expansion rate of the universe is actually increasing, meaning that the
cosmological constant has a positive value. This repulsive gravity — or dark
energy — is actually pushing the universe apart. This is one major feature of
the universe that string theory may be able to explain.
In 1998, two teams of astronomers announced the same results: Studies of
distant supernovas (exploding stars) showed that stars looked dimmer than
expected. The only way to account for this was if the stars were somehow
farther away than expected, but the physicists had already accounted for the
expansion of the universe. The explanation eventually found was startling:
The rate of expansion of the universe was accelerating.
To explain this, physicists realized that there had to be some sort of repulsive
gravity that worked on large scales (see Figure 9-4). On small scales, normal
gravity rules, but on larger scales the repulsive gravity force of dark energy
seemed to take over. (This doesn't contradict the idea that the universe is
flat — but it makes the fact that it is flat, while still expanding, a very unusual
and unexpected set of circumstances, which required very narrow parameters
on the early conditions of our universe.)
y Repulsive gravity
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Repulsive gravity is theorized by inflation theory, but that's a rapid hyper-
expansion in the early phases of the universe. Today's expansion due to dark
energy may be remnants of the repulsive gravity from inflation, or it may be an
entirely distinct phenomenon.
The finding of dark energy (or a positive cosmological constant, which it is
roughly similar to) creates major theoretical hurdles, especially considering
how weak dark energy is. For years, quantum field theory predicted a huge
cosmological constant, but most physicists assumed that some property
_ Chapter 9: Physics in Space: Considering Cosmology and Astrophysics J 33
(such as supersymmetry, which does reduce the cosmological constant
value) canceled it out to zero. Instead, the value is non-zero, but differs from
theoretical predictions by nearly 120 decimal places! (You can find a more
detailed explanation of this discrepancy in Chapter 14.)
In fact, results from the WMAP show that the vast majority of material in our
present universe — about 73 percent — is made up of dark energy (remember
from relativity that matter and energy are different forms of the same thing:
E = mc 2 , after all). The five-year WMAP data, released in 2008 and shown in
Figure 9-5, also allows you to compare the composition of the present
universe with the material present in the universe 13.7 billion years ago. The
dark energy was a vanishingly small slice of the pie 13.7 billion years ago, but
today it eclipses matter and drives the universe's expansion.
Figure 9-5:
The WMAP
data allows
you to com-
pare today's
universe
with the dis-
tant past.
Dark
energy 1
72%
Ordinary matter
(Atoms)
4.6%
""""W"^ Dark
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W \23%
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Today
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v y 12%
13.7 Billion Years Ago
(Universe 380,000 years old)
The history of the universe is a fascinating topic for study, and trying to
understand the meaning of this dark energy is one of the key aspects of
modern cosmology. It's also one of the key challenges to modern variations
of string theory, as you see in Chapter 11.
Today, many string theorists devote attention to these cosmological
mysteries of the universe's origins and evolution because they provide a
universal playground on which the ideas of string theory can be explored,
potentially at energy levels where string behavior may manifest itself. In
Chapters 12, 14, and 15, you discover what behaviors these string theorists
might be looking for and what the implications are for the universe.
Stretching the fabric of Space-lime
into a Black Hole
156
Part II: The Physics Upon Which String Theory Is Built _
One of the consequences of Einstein's general theory of relativity was a
solution in which space-time curved so much that even a beam of light
became trapped. These solutions became called black holes, and the study of
them is one of the most intriguing fields of cosmology. Application of string
theory to study black holes is one of the most significant pieces of evidence
in favor of string theory.
Black holes are believed to form when stars die and their massive bulk
collapses inward, creating intense gravitational fields. No one has "seen" a
black hole, but scientists have observed gravitational evidence consistent
with predictions about them, so most scientists believe they exist.
What goes on inside a btack hole)
According to the general theory of relativity, it's possible that the very fabric
of space-time bends an infinite amount. A point with this infinite curvature is
called a space-time singularity. If you follow space-time back to the big bang,
you'd reach a singularity. Singularities also exist inside of black holes, as
shown in Figure 9-6.
Because general relativity says that the curvature of space-time is equivalent
to the force of gravity, the singularity of a black hole has infinite gravity.
Any matter going into a black hole would be ripped apart by this intense
gravitational energy as it neared the singularity.
For this reason, black holes provide an excellent theoretical testing ground
for string theory. Gravity is normally so weak that quantum effects aren't
observed, but inside of a black hole, gravity becomes the dominant force
at work. A theory of quantum gravity, such as string theory, would explain
exactly what happens inside a black hole.
_ Chapter 9: Physics in Space: Considering Cosmology and Astrophysics / f) /
What qoes on at the edqe of a black hole)
The edge of a black hole is called the event horizon, and it represents a
barrier that even light can't come out of. If you were to go near the edge of
a black hole, relativistic effects take place, including time dilation. To an
outside observer, it would look like time was slowing down for you, eventually
coming to a stop. (You, on the other hand, would notice nothing — until the
black hole's intense gravitational forces squished you, of course.)
It was previously believed that things only get sucked into a black hole, but
physicist Stephen Hawking famously showed that black holes emit an energy
called Hawking radiation. (This was proposed in 1974, a year after the equally
groundbreaking realization by Israeli Jacob Bekenstein that black holes
possessed entropy — a thermodynamic measure of disorder in a system.
The entropy measures the number of different ways to arrange things in a
system.)
Quantum physics predicts that virtual particles are continually created and
destroyed, due to quantum fluctuations of energy in the vacuum. Hawking
applied this concept to black holes and realized that if such a pair is created
near the event horizon, it was possible for one of the particles to get pulled
into the black hole while the other one didn't. This would look identical to the
black hole emitting radiation. To preserve energy, the particle that fell into the
black hole must have negative energy and reduce the overall energy (or mass)
of the black hole.
The behavior of black holes is curious in a number of ways, many of them
demonstrated by Hawking in the 1970s:
K" A black hole's entropy is proportional to the surface area of the black
hole (the area of the event horizon), unlike conventional systems where
entropy is proportional to volume. This was Bekenstein's discovery.
J-" If you put more matter into a black hole, it cools down.
v* As a black hole emits Hawking radiation, the energy comes from the
black hole, so it loses mass. This means the black hole heats up, losing
energy (and therefore mass) more quickly.
i other words, Stephen Hawking showed in the mid-1970s that a black hole
/ill evaporate (unless it is "fed" more mass than it loses in energy). He did this
iy applying principles of quantum physics to a problem of gravity. After the
ilack hole evaporates down to the size of the Planck length, a quantum theory
if gravity is needed to explain what happens to it.
/ yS Part ll: The Physics Upon Which String Theory Is Built _
Hawking's solution is that the black hole evaporates at that point, emitting a
final burst of random energy. This solution results in the so-called black hole
information paradox, because quantum mechanics doesn't allow information
to be lost, but the energy from the evaporation doesn't seem to carry the
information about the matter that originally went into the black hole. I
discuss this black hole information paradox and its potential resolutions in
greater detail in Chapter 14.
Part III
Building String
Theory: A Theory
of Everything
The 5 th Wave
By Rich Tennant
■ZjZvt\% Vb+tf -vary
" VTKat exactly are vre saving here?"
In this part . . .
String theory has existed for nearly four decades. It's
one of the most unusual scientific theories of all time
because it has developed backwards. It began as a theory
of particle interactions and failed at that (only to later
incorporate the theory that replaced it). It then became a
theory of quantum gravity, but made predictions that
didn't seem to match reality.
Today string theory has become so complex and has
yielded so many unexpected results that its proponents
have begun citing this flexibility within the theory as one
of its greatest strengths.
This part explains how string theory got its start and how
it has transformed over the years. I explain the basic
interpretations of key concepts, as well as the ways in
which string theorists have been able to adapt to new
findings. Finally, I look at some ways that scientists might
be able to prove — or disprove — string theory.
Chapter 10
Early Strings and Superstrings:
Unearthing the Theory's
Beginnings
In This Chapter
Knowing how string theory got its start
Focusing on the theory's basic concepts
Saving the science with superstrings and supergravity
Cheering on the first superstring revolution
I\ year before astronauts set foot on the moon, no one had ever heard of
V \ string theory. The concepts at the core of the theory were being neither
discussed nor debated. Physicists struggled to complete the Standard Model
of particle physics, but had abandoned the hopes of a theory of everything
(if they ever had any such hope in the first place).
In other words, no one was looking for strings when physicists found them.
In this chapter, I tell you about the early beginnings of string theory, which
quickly failed to do anything the creators expected (or wanted) it to do.
Then I explain how, from these humble beginnings, several elements of string
theory began to spring up, which drew more and more scientists to pursue it.
Bosonic String Theory:
The First String Theory
The first string theory has become known as bosonic string theory, and it said
that all the particles that physicists have observed are actually the vibration
of multidimensional "strings." But the theory had consequences that made it
unrealistic to use to describe our reality.
162
Part III: Building String Theory: A Theory of Everything _
A dedicated group of physicists worked on bosonic string theory between
1968 and the early 1970s, when the development of superstring theory
(which said the same thing, but fit reality better) supplanted it. (I explain
this superior theory in the later section "Supersymmetry Saves the Day:
Superstring Theory.")
Even though bosonic string theory was flawed and incomplete, string
theorists occasionally do mathematical work with this model to test new
methods and theories before moving on to the more modern superstring
models.
Explaining the scattering of particles
With early dual resonance models
String theory was born in 1968 as an attempt to explain the scattering of
particles (specifically hadrons, like protons and neutrons) within a particle
accelerator. Originally, it had nothing to do with strings. These early
predecessors of string theory were known as dual resonance models.
The initial and final state of particle interactions can be recorded in an array
of numbers called an S-matrix. At the time, finding a mathematical structure
for this S-matrix was considered to be a significant step toward creating a
coherent model of particle physics.
Gabriele Veneziano, a physicist at the CERN particle accelerator laboratory,
realized that an existing mathematical formula seemed to explain the
mathematical structure of the S-matrix. (See the sidebar "Applications of
pure mathematics to physics" for more on this formula.) (Physicist Michio
Kaku has stated that Mahiko Suzuki, also at CERN, made the same discovery
at the same time, but was persuaded by a mentor not to publish it.)
Veneziano's explanation has been called the dual resonance model, the
Veneziano amplitude, or just the Veneziano model. The dual resonance model
was close to the correct result for how hadrons interacted, but not quite
correct. At the time Veneziano developed the model, particle accelerators
weren't precise enough to detect the differences between model and reality.
(Eventually, it would be shown that the alternative theory of quantum
chromodynamics was the correct explanation of hadron behavior, as
discussed in Chapter 8.)
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings / \)j
Applications of pure mathematics to physics
Physicists frequently find the math they need was
created long before it was needed. For example,
the equation that physicist Gabriele Veneziano
used to explain particle scattering was the
Euler beta function, which was discovered
in the 1700s by Swiss mathematician Leonhard
Euler. Also, when Einstein began to extend
special relativity into general relativity, he soon
realized that traditional Euclidean geometry
wouldn't work. His space had to curve, and
Euclid's geometry only described flat surfaces.
Fortunately for Einstein, in the mid-1800s the
German mathematician Bernhard Riemann had
worked on a form of non-Euclidean geometry
(named Riemannian geometry). The mathematics
that Einstein needed for the general theory
of relativity had been created a half century
earlier as an intellectual exercise, with no
practical purpose in mind. (As fascinating as
revolutionizing the foundations of geometry
may be, it was hardly practical.)
This happened several times in the history of
string theory. Calabi-Yau manifolds, discussed
at the end of this chapter, are one example.
Another example is when string theorists
were attempting to determine the appropriate
number of dimensions to make their theories
stable and consistent. A key to this problem
came from the journals of Indian mathematical
genius Srinivasa Ramanujan (referenced in
the film Good Will Hunting), who died in 1920.
The specific mathematics in this case was a
function called the Ramanujan function.
After the dual resonance model was formed, hundreds of theoretical papers
were published in attempts to modify the parameters a bit. This was the way
theories were approached in physics; after all, an initial guess at a theory is
rarely precisely correct and typically requires subtle tweaks — to see how
the theory reacts, how much it can be bent and modified, and so on — so
that ultimately it fits with the experimental results.
The dual resonance model would have nothing to do with that sort of
tinkering — it simply didn't allow for any changes that would still enable it
to be valid. The mathematical parameters of the theory were too precisely
fixed. Attempts to modify the theory in any way quickly led to a collapse of
the entire theory. Like a dagger balanced on its tip, any slight disturbance
would send it toppling over. Mathematically, it was locked into a certain set
of values. In fact, it has been said by some that the theory had absolutely no
adjustable parameters — at least not until it was transformed into an entirely
different concept: superstring theory!
This isn't the way theories are supposed to behave. If you have a theory
and modify it so the particle mass, for example, changes a bit, the theory
shouldn't collapse — it should just give you a different result.
I \)ll Part III: Building String Theory: A Theory of Everything _
When a theory can't be modified, there are only two possible reasons:
either it's completely wrong or it's completely right! For several years, dual
resonance models looked like they might be completely right, so physicists
continued to ponder what they might mean.
Exploring the first physical model:
Particles as strings
The basic physical interpretation of string theory was as vibrating strings.
As the strings, each representing a particle, collided with each other, the
S-matrix described the result.
Consider this very informal way of looking at string theory, shown in Figure
10-1. Each particle is composed of a vibrating string. In the case of a proton,
there are three quark strings. When these three strings come in contact, they
bond together to form a proton. So the proton is created by the interaction
of the three quark strings touching each other. The proton is kind of a knot
within the strings.
What are these strings like? The strings described were almost like rubber
bands. There is a certain "springiness" to them. A phrase that I think
describes them well is "filaments of energy" (as string theorist Brian Greene
and others have called them). Though most people think of particles as balls
of matter, physicists have long thought of them as little bundles of waves
(called wave packets), which is in line with describing them as strings. (In
some other situations, physicists can treat particles as having no size
whatsoever, but this is a simplification to make the math and theory more
manageable. The way physicists treat particles depends a lot on the situation
they're working with.)
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings / %}^
This interpretation was put forth independently by Yoichiro Nambu, Holger
Nielsen, and Leonard Susskind in 1970, earning all three men positions as
founders of string theory.
According to Einstein's work, mass was a form of energy, an insight
demonstrated dramatically by the creation of the atomic bomb. Quantum
theory showed physicists that matter was represented by the mathematics
of wave mechanics, so even a particle had a wavelength associated with it.
In string theory, matter again takes on a new form. Particles of different
types are different vibrational modes of these fundamental entities: energetic
rubber bands, or strings. (Classical vibrations and strings are discussed in
Chapter 5.) In essence, the more the string vibrates, the more energy (and
therefore mass) it possesses.
Through all the transformations that string theory has undergone in the
years since its discovery, this central concept remains (fairly) constant,
although in recent years new objects in addition to strings have been
introduced (which I explain in Chapter 11 when I discuss branes).
The basic physical model couldn't have been simpler: The particles and forces
in nature are really interactions between vibrating strings of energy.
Bosonic string theory loses out
to the Standard Model
The dual resonance model was created for the express purpose of
explaining the S-matrix particle scattering, which was now explained in
terms of the Standard Model of particle physics — gauge fields and
quantum chromodynamics. (See Chapter 8 for more on these concepts.)
There was no point to string theory in light of the success of the Standard
Model.
Also, as the measurements of experiments in particle accelerators got more
precise, it became clear that dual resonance models were only approximately
correct. In 1969, physicists showed that Veneziano had discovered only
the first term in an infinite series of terms. Although this term was the most
important, it still wasn't complete. The theory appeared to need some further
refinement to match the results perfectly.
Terms could be added (which Michio Kaku did in 1972), correcting for the
different ways that the strings could collide, but it made the theory less
elegant. There were growing indications that string theory might not work
the way everyone had thought it would and that, indeed, quantum
chromodynamics explained the behavior of the particle collisions better.
166
Part III: Building String Theory: A Theory of Everything _
The early string theorists had therefore spent a lot of time giving meaning to a
theory that seemed to (almost) accurately predict the S-matrix, only to find that
the majority of particle physicists weren't interested in it. It had to be very
frustrating to have such an elegant model that was quickly falling into obscurity.
But a few string theorists weren't about to give up on it quite yet.
Why Bosonic String Theory Doesn't
Describe Our Universe
By 1974, bosonic string theory was quickly becoming a mathematical mess,
and attempts to make the theory mathematically consistent caused more
trouble for the model than it had already. Playing with the math introduced
four conditions that should have, by all rights, spelled the end of the early
string theory:
w Massless particles
v" Tachyons, which move faster than the speed of light
w Fermions, such as electrons, can't exist
J-" 25 spatial dimensions
The cause of these problems was a reasonable constraint built into string
theory. No matter what else string theory did, it needed to be consistent with
existing physics — namely special relativity and quantum theory.
The Standard Model of particle physics was consistent with both theories
(though it still had trouble reconciling with general relativity), so string
theory also had to be consistent with both. If it violated a half century of
established physics, there was no way it could be a viable theory.
Physicists eventually found ways to modify the theory to be consistent with
these existing physical laws. Unfortunately, these modifications resulted in
the four problematic features outlined in the bulleted list. It wasn't just that
these features were possible, but that they were now seemingly essential
components of the theory.
Massless particles
One side effect of creating a consistent string theory is that it had to contain
certain objects that can never be brought to rest. Because mass is a measure
of an object while it's at rest, these sorts of particles are called massless
particles. This would be a major problem for string theory if the massless
particles predicted didn't really exist.
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings
167
Overall, though, this wasn't a terribly disturbing problem because scientists
know for certain that at least one particle exists only in a state of motion:
the photon. (The gluon, though not known for certain at the time, is also a
massless particle.)
Under the Standard Model of particle physics at the time, it was believed that
a particle called the neutrino might have a mass of zero. (Today we know that
the neutrino's mass is slightly higher than zero.)
There was also one other possible massless particle: the graviton. The
graviton is the theoretical gauge boson that could be responsible for the force
of gravity under quantum field theory.
The existence of massless particles in string theory was unfortunate, but
it was a surmountable problem. String theorists needed to uncover the
properties of massless particles and prove that their properties were
consistent with the known universe.
Tachyons
A bigger problem than massless particles was the tachyon, a particle predicted
by bosonic string theory that travels faster than the speed of light. Under a
consistent bosonic string theory, the mathematical formulas demanded
that tachyons exist, but the presence of tachyons in a theory represents a
fundamental instability in the theory. Solutions that contain tachyons will
always decay into another, lower energy solution — possibly in a never-
ending cycle. For this reason, physicists don't believe that tachyons really
exist, even if a theory initially looks like it contains such particles.
Strictly speaking, Einstein's theory of relativity doesn't absolutely forbid an
object from traveling faster than the speed of light. What it says is that it
would require an infinite amount of energy for an object to accelerate to the
speed of light. Therefore, in a sense, the tachyon would still be consistent with
relativity, because it would always be moving faster than the speed of light
(and wouldn't ever have to accelerate to that speed).
Mathematically, when calculating a tachyon's mass and energy using
relativity, it would contain imaginary numbers. (An imaginary number is
the square root of a negative number.)
This was exactly how string theory equations predicted the tachyon: They
were consistent only if particles with imaginary mass existed. But what is
imaginary mass? What is an imaginary energy? These physical impossibilities
give rise to the problems with tachyons.
The presence of tachyons is in no way unique to bosonic string theory. For
example, the Standard Model contains a certain vacuum in which the Higgs
boson is actually a type of tachyon as well. In this case, the theory isn't
168
Part III: Building String Theory: A Theory of Everything _
inconsistent; it just means that the solution that was applied wasn't a stable
solution. It's like trying to place a ball at the top of a hill — any slight
movement will cause the ball to roll into a nearby valley. Similarly, this
tachyon solution decays into a stable solution without the tachyons.
Unfortunately, in the case of bosonic string theory, there was no clear way to
figure out what happened during the decay, or even if the solution ended up
in a stable solution after decaying into a lower energy state.
With all of these problems, physicists don't view these tachyons as actual
particles that exist, but rather as mathematical artifacts that fall out of the
theory as a sign of certain types of inherent instabilities. Any solution that
contains tachyons quickly decays due to these instabilities.
Some physicists (and science fiction authors) have explored notions of how
to treat tachyons as actual particles, a speculative concept that will come up
briefly in Chapter 16. But for now, just know that tachyons were one of the
things that made physicists decide, at the time, that bosonic string theory
was a failure.
Mo electrons allowed
The real flaw in bosonic string theory was the one that it's named after. The
theory predicted only the existence of bosons, not fermions. Photons could
exist, but not quarks or electrons.
Every elementary particle observed in nature has a property called a spin,
which is either an integer value (-1, 0, 1, 2, and so on) or a half-integer value
(-A, A, and so on). Particles with integer spins are bosons, and particles with
half-integer spins are fermions. One key finding of particle physics is that all
particles fall into one of these two categories.
For string theory to apply to the real world it had to include both types of
particles, and the original formulation didn't. The only particles allowed
under the first model of string theory were bosons. This is why it would
come to be known to physicists as the bosonic string theory.
25 space dimensions, plus 1 of time
Dimensions are the pieces of information needed to determine a precise point
in space. (Dimensions are generally thought of in terms of up/down, left/
right, forward/backward.) In 1974, Claude Lovelace discovered that bosonic
string theory could only be physically consistent if it were formulated in 25
spatial dimensions (Chapter 13 delves into the idea of the additional dimensions
in more depth), but so far as anyone knows, we only have three spatial
dimensions!
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings I Oy
Relativity treats space and time as a continuum of coordinates, so this means
that the universe has a total of 26 dimensions in string theory, as opposed
to the four dimensions it possesses under Einstein's special and general
relativity theories.
It's unusual that this requirement would be implicit in the theory. Einstein's
relativity has three spatial dimensions and one time dimension because
those are the conditions used to create the theory. He didn't begin working
on relativity and just happen to stumble upon three spatial dimensions, but
rather intentionally built it into the theory from the beginning. If he'd wanted
a 2-dimensional or 5-dimensional relativity, he could have built the theory to
work in those dimensions.
With bosonic string theory, the equations actually demanded a certain
number of dimensions to be mathematically consistent. The theory falls
apart in any other number of dimensions!
The reason for extra dimensions
The reason for these extra dimensions can be seen by analogy. Consider
a long, loose spring (like a Slinky), which is flexible and elastic, similar to
the strings of string theory. If you lay the spring in a straight line flat on the
floor and pull it outward, waves move along the length of the spring. These
are called longitudinal waves and are similar to the way sound waves move
through the air.
The key thing is that these waves, or vibrations, move only back and forth
along the length of the spring. In other words, they're 1-dimensional waves.
Now imagine that the spring stays on the floor, but someone holds each end.
Each person can move the ends of the spring anywhere they want, so long
as it stays on the floor. They can move it left and right, or back and forth, or
some combination of the two. As the ends of the spring move in this way, the
waves that are generated require two dimensions to describe the motion.
Finally, imagine that each person has an end of the spring but can move it
anywhere — left or right, back or forth, and up or down. The waves generated
by the spring require three dimensions to explain the motion. Trying to use
2-dimensional or 1-dimensional equations to explain the motion wouldn't
make sense.
In an analogous way, bosonic string theory required 25 spatial dimensions so
the symmetries of the strings could be fully consistent. (Conformal symmetry
is the exact name of the type of symmetry in string theory that requires this
number of dimensions.) If the physicists left out any of those dimensions, it
made about as much sense as trying to analyze the 3-dimensional spring in
only one dimension . . . which is to say, none at all.
/ /(/ Part III: Building String Theory: A Theory of Everything _
Dealing With the extra dimensions
The physical conception of these extra dimensions was (and still is) the
hardest part of the theory to comprehend. Everyone can understand three
spatial dimensions and a time dimension. Give me a latitude, longitude,
altitude, and time, and I can meet you anywhere on the planet. You can
measure height, width, and length, and you experience the passage of time,
so you have a regular familiarity with what those dimensions represent.
What about the other 22 spatial dimensions? It was clear that these dimensions
had to be hidden somehow. The Kaluza-Klein theory predicted that extra
dimensions were rolled up, but rolling them up in precisely the right way to
achieve results that made sense was difficult. This was achieved for string
theory in the mid-1980s through the use of Calabi-Yau manifolds, as I discuss
later in this chapter.
No one has any direct experience with these strange other dimensions.
For the idea to come out of the symmetry relationships associated with a
relatively obscure new theoretical physics conjecture certainly didn't offer
much motivation for physicists to accept it. And for more than a decade,
most physicists didn't.
Supersymmetry Scutes the Day:
Superstring Theory
Despite bosonic string theory's apparent failures, some brave physicists
stayed committed to their work. Why? Well, physicists can be a passionate
bunch (nearly obsessive, some might say). Another reason was that by the
time these problems were fully realized, many string theorists had already
moved on from bosonic string theory anyway.
With the development of supersymmetry in 1971, which allows for bosons
and fermions to coexist, string theorists were able to develop supersymmetric
string theory, or, for short, superstring theory, which took care of the major
problems that destroyed bosonic string theory. This work opened up whole
new possibilities for string theory.
Almost every time you hear or read the phrase "string theory," the person
probably really means "superstring theory." Since the discovery of
supersymmetry, it has been applied to virtually all forms of string theory.
The only string theory that really has nothing to do with supersymmetry
is bosonic string theory, which was created before supersymmetry. For all
practical discussion purposes (with anyone who isn't a theoretical physicist),
"string theory" and "superstring theory" are the same term.
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings / / /
Fermions and bosons coexist . . . sort of
Symmetries exist throughout physics. A symmetry in physics is basically any
situation where two properties can be swapped throughout the system and
the results are precisely the same.
The notion of symmetry was picked up by Pierre Ramond in 1970, followed
by the work of John Schwarz and Andre Neveu in 1971, to give hope to string
theorists. Using two different techniques, they showed that bosonic string
theory could be generalized in another way to obtain non-integer spins. Not
only were the spins non-integer, but they were precisely half-integer spins,
which characterize the fermion. No spin K particles showed up in the theory,
which is good because they don't exist in nature.
Including fermions into the model meant introducing a powerful new
symmetry between fermions and bosons, called supersymmetry.
Supersymmetry can be summarized as
Iu* Every boson is related to a corresponding fermion.
k" Every fermion is related to a corresponding boson.
In Chapter 11,1 discuss the reasons to believe that supersymmetry is true,
as well as ways that it can be proved. For now, it's enough to know that it's
needed to make string theory work.
Who discovered supersymmetry?
The origins of supersymmetry are a bit
confusing, because it was discovered around
the same time by four separate groups.
In 1971, Russians Evgeny Likhtman and Yuri
Golfand created a consistent theory containing
supersymmetry. A year later, they were
followed by two more Russians, Vladimir Akulov
and Dmitri Volkov. These theories were in only
two dimensions, however.
Due to the Cold War, communication between
Russia and the non-communist world wasn't
very good, so many physicists didn't hear about
the Russian work. European physicists Julius
Wess and Bruno Zumino were able to create a
4-dimensional supersymmetric quantum theory
in 1973, probably aware of the Russian work.
Theirs was noticed by the Western physics
community at large.
Then, of course, we have Pierre Ramond, John
Schwarz, and Andre Neveu, who developed
supersymmetry in 1970 and 1971, in the context
of their superstring theories. It was only on
later analysis that physicists realized their work
and the later work hypothesized the same
relationships.
Many physicists consider this repeated
discovery as a good indication that there's prob-
ably something to the idea of supersymmetry
in nature, even if string theory itself doesn't
prove to be correct.
/ (£ P art '" : Building String Theory: A Theory of Everything _
Of course, as you'll anticipate if you're looking for trends in the story of
string theory, things didn't quite fall out right. Fermions and bosons have
very different properties, so getting them to change places without affecting
the possible outcomes of an experiment isn't easy.
Physicists know about a number of bosons and fermions, but when they
began looking at the properties of the theory, they found that the
correspondence didn't exist between known particles. A photon (which is a
boson) doesn't appear to be linked by supersymmetry with any of the known
fermions.
Fortunately for theoretical physicists, this messy experimental fact was seen
as only a minor obstacle. They turned to a method that has worked for
theorists since the dawn of time. If you can't find evidence of your theory,
hypothesize it!
Double your particle fun: Supersymmetry
hypothesizes superpartners
Under supersymmetry, the corresponding bosons and fermions are called
superpartners. The superpartner of a standard particle is called a sparticle.
Because none of the existing particles are superpartners, this means that
if supersymmetry is true, there are twice as many particles as we currently
know about. For every standard particle, a sparticle that has never been
detected experimentally must exist. The detection of sparticles will be one of
the key pieces of evidence the Large Hadron Collider will look for.
If I mention a strangely named particle that you've never run into, it's probably
a sparticle. Because supersymmetry introduces so many new particles, it's
important to keep them straight. Physicists have introduced a Dr. Seuss-like
naming convention to identify the hypothetical new particles:
If-" The superpartner of a fermion begins with an "s" before the standard
particle name; so the superpartner of an "electron" is the "selectron,"
and the superpartner of the "quark" is the "squark."
(^ The superpartner of a boson ends in an "-ino," so the superpartner of a
"photon" is the "photino" and of the "graviton" is the "gravitino."
Table 10-1 shows the names of standard particles and their corresponding
superpartner.
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings / {j
Table 10-1
Some Superpartner Names
Standard Particle
Superpartner
Lepton
Slepton
Muon
Smuon
Neutrino
Sneutrino
Top Quark
Stop Squark
Gluon
Gluino
Higgs boson
Higgsino
W boson
Wino
Z boson
Zino
Even though there is an elementary superpartner called a "sneutrino," there
exists no elementary particle called a "sneutron."
Some problems get fixed, but the
dimension problem remains
The introduction of supersymmetry into string theory helped with some of
the major problems of bosonic string theory. Fermions now existed within
the theory, which had been the biggest problem. Tachyons vanished from
superstring theory. Massless particles were still present in the theory, but
weren't seen as a major issue. Even the dimensional problem improved,
dropping from 26 space-time dimensions down to a mere ten.
The supersymmetry solution was elegant. Bosons — the photon, graviton,
Z, and W bosons — are units of force. Fermions — the electron, quarks, and
neutrinos — are units of matter. Supersymmetry created a new symmetry,
one between matter and forces.
In 1972, Andre Neveu and Joel Scherk resolved the massless particle issue by
showing that string vibrational states could correspond to the gauge bosons,
such as the massless photon.
/ (11 Part III: Building String Theory: A Theory of Everything _
The dimensional problem remained, although it was better than it had been.
Instead of 25 spatial dimensions, superstring theory became consistent with
a "mere" nine spatial dimensions (plus one time dimension, for a total of ten
dimensions). Many string theorists of the day believed this was still too many
dimensions to work with, so they abandoned the theory for other lines of
research.
One physicist who turned his back on string theory was Michio Kaku, one of
today's most vocal advocates of string theory. Kaku's PhD thesis involved
completing all the terms in the Veneziano model's infinite series. He'd created
a field theory of strings, so he was working in the thick of string theory. Still,
he abandoned work on superstring theory, believing that there was no way it
could be a valid theory. That's how serious the dimensional problem was.
For the handful of people who remained dedicated to string theory after 1974,
they faced serious issues about how to proceed. With the exception of the
dimensional problem, they had resolved nearly all the issues with bosonic
string theory by transforming it into superstring theory.
The only question was what to do with it.
Supersymmetry and Quantum
Gravity in the Disco Era
By 1974, the Standard Model had become the theoretical explanation of
particle physics and was being confirmed in experiment after experiment.
With a stable foundation, theoretical physicists now looked for new worlds
to conquer, and many decided to tackle the same problem that had vexed
Albert Einstein for the last decades of his life: quantum gravity.
Also as a consequence of the Standard Model's success, string theory wasn't
needed to explain particle physics. Instead, almost by accident, string
theorists began to realize that string theory might just be the very theory
that would solve the problem of quantum gravity.
The qraViton is found hiding
in string theory
The graviton is a particle that, under predictions from unified field theory,
would mediate the gravitational force (see Chapter 2 for more on the
graviton). In a very real sense, the graviton is the force of gravity. One
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings / ( j
major finding of string theory was that it not only includes the graviton, but
requires its existence as one of the massless particles discussed earlier in
this chapter.
In 1974, Joel Scherk and John Schwarz demonstrated that a spin-2 massless
particle in superstring theory could actually be the graviton. This particle
was represented by a closed string (which formed a loop), as opposed to an
open string, where the ends are loose. Both sorts of strings are demonstrated
in Figure 10-2.
Figure 10-2:
String the-
ory allows
for open
and closed
strings.
Open strings
are optional,
but closed
strings have
to exist.
String theory demands that these closed strings must exist, though open
strings may or may not exist. Some versions of string theory are perfectly
mathematically consistent but contain only the closed strings. No theory
contains only open strings, because if you have open strings, you can construct
a situation where the ends of the strings meet each other and, voila, a closed
string exists. (Cutting closed strings to get open strings isn't always allowed.)
From a theoretical standpoint, this was astounding (in a good way). Instead
of trying to shoehorn gravity into the theory, the graviton fell out as a natural
consequence. If superstring theory was the fundamental law of nature, then it
required the existence of gravity in a way that no other proposed theory had
ever done!
Immediately, it became clear to Schwarz and Scherk that they had a potential
candidate for quantum gravity on their hands.
Even while everyone else was fleeing from the multiple dimensions their
theory predicted, Scherk and Schwarz became more convinced than ever
that they were on the right track.
176
Part III: Building String Theory: A Theory of Everything _
The other supersymmetric gravity
theory: Supergravity
Supergravity is the name for theories that attempt to apply supersymmetry
directly to the theory of gravity without the use of string theory. Throughout
the late 1970s, this work proceeded at a faster pace than string theory,
mainly because it was popular while the string theory camp had become a
ghost town. Supergravity theories prove important in the later development
of M-theory, which I cover in Chapter 11.
In 1976, Daniel Freedman, Sergio Ferrara, and Peter van Nieuwenhuizen
applied supersymmetry to Einstein's theory of gravity, resulting in a theory
of supergravity. They did this by introducing the superpartner of the
graviton, the gravitino, into the theory of general relativity.
Building on this work, Eugene Cremmer, Joel Scherk, and Bernard Julia were
able to show in 1978 that supergravity could be written, in its most general
form, as an 11-dimensional theory. Supergravity theories with more than 11
dimensions fell apart.
Supergravity ultimately fell prey to the mathematical inconsistencies that
plagued most quantum gravity theories (it worked fine as a classical theory,
so long as you kept it away from the quantum realm), leaving room for
superstring theory to rise again in the mid-1980s, but it didn't go away
completely. I return to the idea of the 1 1-dimensional supergravity theory in
Chapter 11.
String theorists don't get no respect
During the late 1970s, string theorists were finding it hard to be taken
seriously, let alone find secure academic work. String theorists' search for
respect in the field of physics reminds me of a young Einstein working in
the Bern patent office, denied job after job while he thought about mass and
energy.
There had been earlier issues in getting recognition for string theory work.
The journal Physics Review Letters didn't consider Susskind's 1970 work —
interpreting the dual resonance model as vibrating strings — significant
enough to publish. Susskind himself tells how physics giant Murray Gell-
Mann laughed at him for mentioning string theory in 1970. (The story ends
well, with Gell-Mann expressing interest in the theory in 1972.)
As the decade progressed, two of the major forces behind string theory
would run into hurdle after hurdle in getting a secure professorship. John
Schwarz had been denied tenure at Princeton in 1972 and spent the next 12
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings 7 / /
years at CalTech in a temporary position, never sure if the funding for his job
would be renewed. Pierre Ramond, who had discovered supersymmetry and
helped rescue string theory from oblivion, was denied tenure at Yale in 1976.
Against the backdrop of professional uncertainty, the few string theorists
continued their work through the late 1970s and early 1980s, helping deal
with some of the extra dimensional hurdles in supergravity and other
theories, until the day came when the tables turned and they were able
to lay claim to the high ground of theoretical physics.
A Theory of Everything: The First
Superstring Revolution
The year 1984 is marked by many as the start of "the first superstring
revolution." The major finding that sparked the revolution was the proof that
string theory contained no anomalies, unlike many of the quantum gravity
theories, including supergravity, studied during the 1970s.
For nearly a decade, John Schwarz had been working on showing that
superstring theory could be a quantum theory of gravity. His major partner
in this, Joel Scherk, had died in 1980, a tragic blow to the cause. By 1983,
Schwarz was working with Michael Green, one of the few individuals who had
been persuaded to work on string theory during that time.
Typically, two major problems arose in theories of quantum gravity:
anomalies and infinities. Neither is a good sign for a scientific theory.
IJ-" Infinities occur when values, such as energy, probability, or curvature,
begin increasing rapidly to an infinite value,
v" Anomalies are cases where quantum mechanical processes can violate
a symmetry that is supposed to be preserved.
Superstring theory was actually pretty good at avoiding infinities.
One simplification that allows you to understand, in very general terms, how
superstring theory avoids infinities is that the distance value never quite
reaches zero. Dividing by zero (or a value that can get arbitrarily close to
zero) is the mathematical operation that results in an infinity. Because the
strings have a tiny bit of length (I call it L), the distance never gets smaller
than L, and so the gravitational force is obtained by dividing by a number that
never gets smaller than L 2 . This means that the gravitational force will never
explode up to infinity, as happens when the distance approaches zero without
a limit.
/ jo P art '" : Building String Theory: A Theory of Everything _
String theory also had no anomalies (at least under certain specific
conditions), as Schwarz and Green proved in 1984. They showed that certain
10-dimensional versions of superstring theory had exactly the constraints
needed to cancel out all anomalies.
This changed the whole landscape of theoretical physics. For a decade,
superstring theory had been ignored while every other method of creating a
quantum theory of gravity collapsed in upon itself under infinities and
anomalies. Now this discarded theory had risen from the ashes like a
mathematical phoenix — both finite and anomaly free.
Theorists began to think that superstring theory had the potential to unify
all the forces of nature under one simple set of physical laws with an elegant
model in which everything consisted of different energy levels of vibrating
strings. It was the ideal that had eluded Einstein: a fundamental theory of all
natural law that explained all observed phenomena.
But We've Got Five Theories!
In the wake of 1984's superstring revolution, work on string theory reached
a fever pitch. If anything, it proved a little too successful. It turned out that
instead of one superstring theory to explain the universe, there were five,
given the colorful names
I W Type I
Iv* Type HA
iS Type IIB
V Type HO
iS Type HE
And, once again, each one almost matched our world . . . but not quite.
By the time the decade ended, physicists had developed and dismissed many
variants of string theory in the hopes of finding the one true formulation of
the theory.
Instead of one formulation, though, five distinct versions of string theory
proved to be self-consistent. Each had some properties that made physicists
think it would reflect the physical reality of our world — and some properties
that are clearly not true in our universe.
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings / ( y
The distinctions between these theories are mathematically sophisticated.
I introduce their names and basic definitions mainly because of the key role
they play in M-theory, which I introduce in Chapter 11.
Type 1 string theory
Type /string theory involves both open and closed strings. It contains a form
of symmetry that's mathematically designated as a symmetry group called
0(32). (I'll try to make that the most mathematics you need to know related
to symmetry groups.)
Type UA string theory
Type IIA string theory involves closed strings where the vibrational patterns
are symmetrical, regardless of whether they travel left or right along the
closed string. Type IIA open strings are attached to structures called
D-branes (which I discuss in greater detail in Chapter 11) with an odd number
of dimensions.
Type UB string theory
Type IIB string theory involves closed strings where the vibrational patterns
are asymmetrical, depending upon whether they travel left or right along the
closed string. Type IIB open strings are attached to D-branes (discovered in
1995 and covered in Chapter 11) with an even number of dimensions.
Two strings in one: Heterotic strings
A new form of string theory, called heterotic string theory, was discovered in
1985 by the Princeton team of David Gross, Jeff Harvey, Emil Martinec, and
Ryan Rohm. This version of string theory sometimes acted like bosonic string
theory and sometimes acted like superstring theory.
A distinction of the heterotic string is that the string vibrations in different
directions resulted in different behaviors. "Left-moving" vibrations resembled
the old bosonic string, while "right-moving" vibrations resembled the Type
II strings. The heterotic string seemed to contain exactly the properties that
Green and Schwarz needed to cancel out anomalies within the theory.
/ q (/ Part III: Building String Theory: A Theory of Everything _
d&ST(/± It was ultimately shown that only two mathematical symmetry groups could
^?/»S»\ be applied to heterotic string theory, which resulted in stable theories in ten
dimensions — 0(32) symmetry and E 8 x E 8 symmetry. These two groups gave
rise to the names Type HO and Type HE string theory.
Type HO string theory
Type HO is a form of heterotic string theory. The name comes from the longer
name Heterotic 0(32) string theory, which describes the symmetry group
of the theory. It contains only closed strings whose right-moving vibrations
resemble the Type II strings and whose left-moving vibrations resemble the
bosonic strings. The similar theory, Type HE, has subtle but important
mathematical differences regarding the symmetry group.
Type HE string theory
Type HE is another form of heterotic string theory, based on a different
symmetry group from the Type HO theory. The name comes from the longer
name Heterotic E 8 x E 8 string theory, based on the symmetry group of the
theory. It also contains only closed strings whose right-moving vibrations
resemble the Type II strings and whose left-moving vibrations resemble the
bosonic strings.
HouS to Fold Space: Introducing
Catabi*\lau Manifolds
The problem of extra dimensions continued to plague string theory, but
these were solved by introducing the idea of compactification, in which the
extra dimensions curl up around each other, growing so tiny that they're
extremely hard to detect. The mathematics about how this might be achieved
had already been developed in the form of complex Calabi-Yau manifolds, an
example of which is shown in Figure 10-3. The problem is that string theory
offers no real way to determine exactly which of the many Calabi-Yau
manifolds is right!
When the extra dimensions were first discovered in the 1970s, it was clear
that they must be hidden in some way. After all, we certainly don't see more
than three spatial dimensions.
One suggestion was the one that had been proposed by Kaluza and Klein a
half century earlier: The dimensions could be curled up into a very small size.
Early attempts to curl up these extra dimensions ran into problems because
they tended to retain the symmetry between left- and right-handed particles
(called parity by physicists), which isn't always retained in nature. This
violation is crucial in understanding the operation of the weak nuclear force.
Chapter 10: Early Strings and Superstrings: Unearthing the Theory's Beginnings / q /
For string theory to work, there had to be a way to compactify the extra six
dimensions while still retaining a distinction between the left-handed and
right-handed particles.
In 1985, the Calabi-Yau manifolds (created for other purposes years earlier by
mathematicians Eugenio Calabi and Shing-Tung Yau) were used by Edward
Witten, Philip Candelas, Gary Horowitz, and Andrew Strominger to compactify
the extra six space dimensions in just the right way. These manifolds not only
preserved the handedness of the particles, but they also preserved super-
symmetry just enough to replicate certain aspects of the Standard Model.
One benefit of the Calabi-Yau manifolds was that the geometry of the folded
dimensions gives rise to different types of observable particles in our
universe. If the Calabi-Yau shape has three holes (or rather higher-
dimensional analogs of holes), three families of particles will be predicted
by the Standard Model of particle physics. (Obviously, by extension, a shape
with five holes will have five families, but physicists are only concerned with
the three families of particles that they know exist in this universe.)
Unfortunately, there are tens of thousands of possible Calabi-Yau manifolds
for six dimensions, and string theory offers no reasonable means of
determining which is the right one. For that matter, even if physicists
could determine which one was the right one, they'd still want to answer
the question of why the universe folded up the extra six dimensions in that
particular configuration.
When Calabi-Yau manifolds were first discovered, it was hoped by some
vocal members of the string theory community that one specific manifold
would fall out as the right one. This hasn't proved to be the case, and this is
what many string theorists would have expected in the first place — that the
specific Calabi-Yau manifold is a quantity that has to be determined by
experiment. In fact, it's now known that some other geometries for folded
spaces can also maintain the needed properties. I talk about the implications
of this folded space — what it could really mean — in Chapters 13 and 14.
/ q£ Part III: Building String Theory: A Theory of Everything _
String Theory Loses Steam
The rising tide of string theory research couldn't last forever, and by the
early 1990s some were giving up any hope of finding one single theory. Just
as the earlier introduction of multiple dimensions had warded off new
physicists, the rise of so many distinct yet consistent versions of string
theory gave many physicists pause. Physicists who were motivated purely by
the drive to find a quick and easy "theory of everything" began turning away
from string theory when it became clear that there was nothing quick and
easy about it. As the easier problems got solved and only the harder ones
remained, the truly dedicated retained the motivation to work through the
complications.
In 1995, a second string theory revolution would come along, with the rise
of new insights that would help convince even many of the skeptics that
work on string theory would ultimately bear significant fruit. That second
revolution is the topic of Chapter 11.
Chapter 11
M-Theory and Beyond: Bringing
String Theory Together
In This Chapter
M-theory re-energizes the movement
Thinking about branes
Overcoming the conundrum of dark energy
So many string theories, why pick just one?
T
m he last chapter ended with five versions of string theories. Theorists
P continued their work, but were uncertain how to take these findings. A
new insight was needed to generate further progress in the field.
In this chapter, I explain how that insight came about in the form of M-theory,
which unified these string theories into one theory. I discuss how string
theory was expanded to include objects with more than one dimension,
called branes. I introduce some possible insights that may help explain what
M-theory is trying to describe. I show how the discovery of dark energy,
unpredicted by string theory, has complicated string theory, as well as
introduced a large number of possible correct solutions to the theories.
Finally, I examine how some physicists have used the anthropic principle to
try to give meaning to this landscape of string theories.
Introducing the Unifying Theory:
M-Theory
At a conference in 1995, physicist Edward Witten proposed a bold resolution
to the problem of five distinct string theories. In his theory, based on newly
discovered dualities, each of the existing theories was a special case of one
overarching string theory, which he enigmatically called M-theory. One of the
key concepts required for M-theory was the introduction of branes (short
for membranes) into string theory. Branes are fundamental objects in string
theory that have more than one dimension.
/ o(l Part III: Building String Theory: A Theory of Everything _
Witten didn't thoroughly explain the true meaning of the name M-theory,
leaving it as something that each person can define for himself. There are
several possibilities for what the "M" could stand for: membrane, magic,
mother, mystery, or matrix. Witten probably took the "M" from membrane
because those featured so prominently in the theory, but he didn't want to
commit himself to requiring them so early in the development of the new
theory.
Although Witten didn't propose a complete version of M-theory (in fact, we're
still waiting on one), he did outline certain defining traits that M-theory would
have:
IJ-" 11 dimensions (10 space dimensions plus 1 time dimension)
J-" Dualities that result in the five existing string theories all being different
explanations of the same physical reality
\* Branes — like strings, but with more than one dimension
Translating one string theory
into another: Duality
The core of M-theory is the idea that each of the five string theories
introduced in Chapter 10 is actually a variation on one theory. This new
theory — M-theory — is an 1 1-dimensional theory that allows for each of
the existing theories (which are 10-dimensional) to be equivalent if you
make certain assumptions about the geometry of the space involved.
The basis for this suggestion was the understanding of dualities that were
being recognized among the various string theories. A duality occurs when
you can look at the same phenomenon in two distinct ways, taking one
theory and mapping it to another theory. In a sense, the two theories are
equivalent. By the mid-1990s, growing evidence showed that at least two
dualities existed between the various string theories; they were called
T-duality and S-duality.
These dualities were based on earlier dualities conjectured in 1977 by Claus
Montonen and David Olive. In the early 1990s, Indian physicist Ashoke Sen
and Israeli-born physicist Nathan Seiberg did work that expanded on the
notions of these dualities. Witten drew upon this work, as well as more recent
work by Chris Hull, Paul Townsend, and Witten himself, to present M-theory.
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together / Qj
Topology: The mathematics of folding space
The study of topology allows you to study
mathematical spaces by eliminating all details
from the space except for certain sets of
properties that you care about. Two spaces
are topologically equivalent if they share these
properties, even if they differ in other details.
Certain actions may be more easily performed
on one of the spaces than the other. You then
perform actions on that space and can work
backward to find the resulting effect on the
topologically equivalent space. It can be far
easier than trying to perform these actions on
the original space directly.
One of the key components of topology is the
study of how different topological spaces
relate to each other. Much of the time, these
different spaces involve some sort of manipulation
of the space, which is what adds the complexity.
If this manipulation can be performed without
breaking or reconnecting the space in a
new way, the two spaces are topologically
equivalent.
To picture this, imagine a donut(ortorus)of clay
that you slowly and meticulously recraft into the
shape of a coffee mug. The hole in the center of
the donut never has to be broken in order to be
turned into the handle of the coffee mug. On the
other hand, if you start with a donut, there's no
way to turn it into a pretzel without introducing
breaks into the space — a donut and a pretzel
are topologically distinct.
Topological duality: T-duality
One of the dualities discovered at the time was called T-duality, which refers
to either topological duality or toroidal duality, depending on whom you
ask. (Toroidal is a reference to the simplest case, which is a torus, or donut
shape. Topological is a precise way of defining the structure of that space,
as explained in the nearby sidebar "Topology: The mathematics of folding
space." In some cases the T-duality has nothing to do with a torus, and in
other cases, it's not topological.) The T-duality related the Type II string
theories to each other and the heterotic string theories to each other,
indicating that they were different manifestations of the same fundamental
theory.
In the T-duality, you have a dimension that is compactified into a circle (of
radius R), so the space becomes something like a cylinder. It's possible for
a closed string to wind around the cylinder, like thread on a spindle. (This
means that both the dimension and the string have radius R.~) The number
of times the closed string winds around the cylinder is called the winding
number. You have a second number that represents the momentum of the
closed string.
186
Part III: Building String Theory: A Theory of Everything _
Here's where things get interesting. For certain types of string theory, if you
wrap one string around a cylindrical space of radius R and the other around a
cylindrical space of radius 1/R, then the winding number of one theory seems
to match the momentum number (momentum, like about everything else, is
quantized) of the other theory.
In other words, T-duality can relate a string theory with a large compactified
radius to a different string theory with a small compactified radius (or,
alternately, wide cylinders with narrow cylinders). Specifically, for closed
strings, T-duality relates the following types of string theories:
u* Type IIA and Type IIB superstring theories
u* Type HO and Type HE superstring theories
The case for open strings is a bit less clear. When a dimension of superstring
space-time is compactified into a circle, an open string doesn't wind around
that dimension, so its winding number is 0. This means that it corresponds
to a string with momentum — a stationary string — in the dual superstring
theory.
The end result of T-duality is an implication that Type IIA and IIB superstring
theories are really two manifestations of the same theory, and Type HO and
HE superstring theories are really two manifestations of the same theory.
Strong-Weak duality: S-duatity
Another duality that was known in 1995 is called S-duality, which stands for
strong-weak duality. The duality is connected to the concept of a coupling
constant, which is the value that tells the interaction strength of the string
by describing how probable it is that the string will break apart or join with
other strings.
The coupling constant, g, in string theory describes the interaction strength
due to a quantity known as the dilation field, §. If you had a high positive
dilation field §, the coupling constant g = e§ becomes very large (or the theory
becomes strongly coupled). If you instead had a dilation field -§, the coupling
constant g = er§ becomes very small (or the theory becomes weakly coupled).
Because of the mathematical methods (see nearby sidebar "Perturbation
theory: String theory's method of approximation") that string theorists have
to use to approximate the solutions to string theory problems, it was very
hard to determine what would happen to string theories that were strongly
coupled.
In S-duality, a strong coupling in one theory relates to a weak coupling in
another theory, in certain conditions. In one theory, the strings break apart
and join other strings easily, while in the other theory they hardly ever do
so. In the theory where the strings break and join easily, you end up with a
chaotic sea of strings constantly interacting.
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together / q/
_^- ST o A/>
Trying to follow the behavior of individual strings is similar to trying to follow
the behavior of individual water molecules in the ocean — you just can't do it.
So what do you do instead? You look at the big picture. Instead of looking at
the smallest particles, you average them out and look at the unbroken surface
of the ocean, which, in this analogy, is the same as looking at the strong
strings that virtually never break.
S-duality introduces Type I string theory to the set of dual theories that T-duality
started. Specifically, it shows that the following dualities are related to each other:
(-" Type I and Type HO superstring theories
I i^ Type IIB is S-dual to itself
If you have a Type I superstring theory with a very strong coupling constant,
it's theoretically identical to a Type HO superstring theory with a very weak
coupling constant. So these two types of theories, under these conditions,
yield the exact same predictions for masses and charges.
Perturbation theory: String theory's
method of approximation
The equations of string theory are incredibly
complex, sothey often can only be solved through
a mathematical method of approximation
called perturbation theory. This method is
used in quantum mechanics and quantum field
theory all the time and is a well-established
mathematical process.
In this method, physicists arrive at a first-order
approximation, which is then expanded with
other terms that refine the approximation. The
goal is that the subsequent terms will become
so small so quickly that they'll cease to matter.
Adding even an infinite number of terms will
result in converging onto a given value. In
mathematical speak, converging means that
you keep getting closer to the number without
ever passing it.
Consider the following example of convergence:
If you add a series effractions, starting with Vi
and doubling the denominator each time, and
you added them all together (14 + %% + ... well,
you get the idea), you'll always get closer to a
value of 1, but you'll never quite reach 1. The
reason for this is that the numbers in the series
get small very quickly and stay so small that
you're always justa little bit short of reaching 1.
However, if you add numbers that double (2 +
4 + 8 + . . . well, you get the idea), the series
doesn't converge at all. The solution keeps
getting bigger as you add more terms. In this
situation, the solution is said to diverge or
become infinite.
The dual resonance model that Veneziano
originally proposed — and which sparked
all of string theory — was found to be only a
first-order approximation of what later came to
be known as string theory. Work over the last
40 years has largely been focused on trying to
find situations in which the theory built around
this original first-order approximation can be
absolutely proved to be finite (or convergent),
and which also matches the physical details
observed in our own universe.
/ QQ Part III: Building String Theory: A Theory of Everything _
Using two dualities to unite
five superstring theories
Both T-duality and S-duality relate different string theories together. Here's a
review of the existing string theory relationships:
(^ Type I and Type HO superstring theories are related by S-duality.
Iu* Type HO and Type HE superstring theories are related by T-duality.
J-" Type IIA and Type IIB superstring theories are related by T-duality.
With these dualities (and other, more subtle ones, which relate IIA and IIB
together with the heterotic string theories), relationships exist to transform
one version of string theory into another one — at least for certain specially
selected string theory conditions.
wfcJflBEfl To solve these equations of duality, certain assumptions have to be made,
' /JT\ and not all of them are necessarily valid in a string theory that would describe
IHjj ) our own universe. For example, the theories can only be proved in cases of
perfect supersymmetry, while our own universe exhibits (at best) broken
supersymmetry.
String theory skeptics aren't convinced that these dualities in some specific
states of the theories relate to a more fundamental duality of the theories at
all levels. Physicist (and string theory skeptic) Lee Smolin calls this the
pessimistic view, while calling the string theory belief in the fundamental
nature of these dualities the optimistic view.
Still, in 1995 it was hard not to be in the optimistic camp (and, in fact, many
had never stopped being optimistic about string theory). The very fact
that these dualities existed at all was startling to string theorists. It wasn't
planned, but came out of the mathematical analysis of the theory. This was
seen as powerful evidence that string theory was on the right track. Instead
of falling apart into a bunch of different theories, superstring theory was
actually pulling back together into one single theory — Edward Witten's
M-theory — which manifested itself in a variety of ways.
The second superstring resolution begins:
Connecting to the 1 1 -dimensional theory
The period immediately following the proposal of M-theory has been called
the "second superstring revolution," because it once again inspired a flurry
of research into superstring theory. The research this time focused on
understanding the connections between the existing superstring theories
and between the 11-dimensional theory that Witten had proposed.
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together I Qy
Witten wasn't the first one to propose this sort of a connection. The idea of
uniting the different string theories into one by adding an 1 1th dimension had
been proposed by Mike Duff of Texas A&M University, but it never caught on
among string theorists. Witten's work on the subject, however, resulted in a
picture where the extra dimension could emerge from the unifications
inherent in M-Theory — one that prompted the string theory community to
look at it more seriously.
In 1994, Witten and colleague Paul Townsend had discovered a duality
between the 10-dimensional superstring theory and an 11-dimensional
theory, which had been proposed back in the 1970s: supergravity.
Supergravity resulted when you took the equations of general relativity and
applied supersymmetry to them. In other words, you introduced a particle
called the gravitino — the superpartner to the graviton — to the theory. In
the 1970s this was pretty much the dominant approach to trying to get a
theory of quantum gravity.
What Witten and Townsend did in 1994 was take the 11-dimensional super-
gravity theory from the 1970s and curl up one of the dimensions. They then
showed that a membrane in 1 1 dimensions that has one dimension curled up
behaves like a string in 10 dimensions.
Again, this is a recurrence of the old Kaluza-Klein idea, which comes up again
and again in the history of string theory. By taking Kaluza's idea of adding an
extra dimension (and Klein's idea of rolling it up very small), Witten showed
that it was possible — assuming certain symmetry conditions — to show that
dualities existed between the existing string theories.
There were still issues with an 1 1-dimensional universe. Physicists had
shown supergravity didn't work because it allowed infinities. In fact, every
theory except string theory allowed infinities. Witten, however, wasn't
concerned about this because supergravity was only an approximation of
M-theory, and M-theory would, by necessity, have to be finite.
It's important to realize that neither Witten nor anyone else proved that all
five string theories could be transformed into each other in our universe. In
fact, Witten didn't even propose what M-theory actually was.
What Witten did in 1995 was provide a theoretical argument to support the
idea that there could be a theory — which he called M-theory — that united
the existing string theories. Each known string theory was just an approximation
of this hypothetical M-theory, which was not yet known. At low energy levels,
he also believed that M-theory was approximated by the 1 1-dimensional
supergravity theory.
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Branes: Stretching Out a String
In a sense, the introduction of M-theory marks the end of "string theory,"
because it ceases to be a theory that contains only fundamental strings.
M-theory also contains multidimensional membranes, called branes. Strings
are only 1-dimensional objects, and therefore only one of the types of
fundamental objects that make up the universe, according to the new
M-Theory.
Branes have at least three key traits:
IJ-" Branes exist in a certain number of dimensions, from zero to nine,
j-" Branes can contain an electrical charge.
i^ Branes have a tension, indicating how resistant they are to influence or
interaction.
String theory became more complex with the introduction of multidimensional
branes. The first branes, called D-branes, entered string theory in 1989.
Another type of brane, called a p-brane (not to be confused with the term you
used to tease your younger sibling with), was later introduced. Later work
showed that these two types of branes were in fact the same thing.
Branes are objects of multiple dimensions that exist within the full 10-
dimensional space required by string theory. In the language of string
theorists, this full space is called the bulk.
One major reason that string theorists didn't originally embrace branes was
because introducing more elaborate physical objects went against the goal
of string theory. Instead of simplifying the theory and making it more
fundamental, branes made the theory more complicated and introduced
more types of objects that didn't appear to be necessary. These were the
exact features of the Standard Model that string theorists hoped to avoid.
In 1995, though, Joe Polchinski proved that it wasn't possible to avoid them.
Any consistent version of M-theory had to include higher-dimensional
branes.
The discovery of D-branes: Giving open
strings something to hold on to
The motivation for D-branes came from work by Joe Polchinski, Jin Dai, and
Rob Leigh of the University of Texas, and independent work performed at the
same time by Czech physicist Petr HoFava. While analyzing the equations of
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together I y /
string theory, these physicists realized that the ends of open strings didn't
just hover out in empty space. Instead, it was as if the end of the open string
was attached to an object, but string theory at the time didn't have objects
(other than strings) for it to attach to.
To solve this problem, the physicists introduced the D-brane, a surface that
exists within the 10-dimensional superstring theory so open strings can
attach to them. These branes, and the strings attached to them, are shown
in Figure 1 1-1. (The "D" in D-brane comes from Johann Peter Gustav Lejeune
Dirichlet, a German mathematician whose relationship to the D-brane comes
from a special type of boundary condition, called the Dirichlet boundary
condition, which the D-branes exhibit.)
It's easiest to visualize these branes as flat planes, but the D-branes can exist
in any number of dimensions from zero to nine, depending on the theory. A
5-dimensional D-brane would be called a D5-brane.
It's easy to see how quickly these D-branes can multiply. You could have a
D5-brane intersecting a D3-brane, which has a Dl-brane extending off of it.
Open superstrings could have one end on the Dl-brane and the other end on
the D5-brane, or on some other D5-brane in another position, and D9-branes
(extended in all nine dimensions of space-time) could be in the background
of all of them. At this point, it's clear that it begins to be quite difficult to
picture this 10-dimensional space or keep all the possible configurations
straight in any meaningful way.
In addition, the D-branes can be either finite or infinite in size. Scientists
honestly don't know the real limitations of how these branes behave. Prior to
1995, few people paid much attention to them.
7 y£ ' >art '" : Building String Theory: A Theory of Everything
Creating particles from p-branes
In the mid-1990s, Andrew Strominger performed work on another type of
brane, called p-branes, which were solutions to Einstein's general relativity
field equations. The p represents the number of dimensions, which again can
go from zero to nine. (A 4-dimensional p-brane is called a 4-brane.)
The p-branes expanded infinitely far in certain directions but finitely far in
others. In those finite dimensions, they actually seemed to trap anything that
came near them, similar to the gravitational influence of a black hole. This
work has provided one of the most amazing results of string theory — a way
to describe some aspects of a black hole (see the section "Using branes to
explain black holes").
In addition, the p-branes solved one problem in string theory: Not all of the
existing particles could be explained in terms of string interactions. With
the p-branes, Strominger showed that it was possible to create new particles
without the use of strings.
A p-brane can make a particle by wrapping tightly around a very small,
curled-up region of space. Strominger showed that if you take this to the
extreme — picture a region of space that's curled up as small as possible —
the wrapped p-brane becomes a massless particle.
According to Strominger's research with p-branes, not all particles in string
theory are created by strings. Sometimes, p-branes can create particles as
well. This is important because strings alone did not account for all the known
particles.
Deducing that branes are
required by M-theory
Strongly motivated by Edward Witten's proposal of M-theory, Joe Polchinski
began working intently on D-branes. His work proved that D-branes weren't
just a hypothetical construct allowed by string theory, but they were
essential to any version of M-theory. Furthermore, he proved that the
D-branes and p-branes were describing the same objects.
In a flurry of activity that would characterize the second superstring
revolution, Polchinski showed that the dualities needed for M-theory only
worked consistently in cases where the theory also contained higher
dimensional objects. An M-theory that contained only 1-dimensional strings
would be an inconsistent M-theory.
Chapter 11: M-Theory and Beyond: Bringing String Theory Together / yj
Polchinski defined what types of D-branes string theory allows and some of
their properties. Polchinski's D-branes carried charge, which meant that they
interacted with each other through something similar to the electromagnetic
force.
A second property of D-branes is tension. The tension in the D-brane
indicates how easily an interaction influences the D-brane, like ripples
moving across a pool of water. A low tension means a slight disturbance
results in large effects on the D-brane. A high tension means that it's harder
to influence (or change the shape of) the D-brane.
If a D-brane had a tension of zero, then a minor interaction would have a
major result — like someone blowing on the surface of the ocean and parting
it like the Red Sea in The Ten Commandments. An infinite tension would mean
the exact opposite: No amount of work would cause changes to the D-brane.
If you picture a D-brane as the surface of a trampoline, you can more easily
visualize the situation. When the weight of your body lands on a trampoline,
the tension in the trampoline is weak enough that it gives a bit, but strong
enough that it does eventually bounce back, hurling you into the air. If the
tension in the trampoline surface were significantly weaker or stronger,
a trampoline would be no fun whatsoever; you'd either sink until you hit
the ground, or you'd hit a flat, immovable trampoline that doesn't sink (or
bounce) at all.
Together, these two features of the D-branes — charge and tension — meant
that they aren't just mathematical constructs, but are tangible objects in their
own right. If M-theory is true, D-branes have the capacity to interact with
other objects and move from place to place.
Uniting D-branes and p-branes
into one type of brane
Though Polchinski was aware of Strominger's work on p-branes — they
discussed their projects over lunch regularly — both scientists thought
that the two types of branes were distinct. Part of Polchinski's 1995 work
on branes included the realization that they were actually one and the same
object. At energy levels where predictions from string theory and general
relativity match up, the two are equivalent.
It might seem odd that this hadn't occurred to either of the men before
1995, but there was no reason to expect that the two types of branes would
be related to each other. To a layman, they sound basically the same —
multidimensional surfaces existing in a 10-dimensional space-time. Why
wouldn't you at least consider that they're the same things?
7 yli P art '" : Building String Theory: A Theory of Everything _
Well, part of the reason may be based on the specific nature of scientific
research. When you're working in a scientific field, you are quite specific
about the questions you're asking and the ways in which you're asking them.
Polchinski and Strominger were asking different questions in different ways,
so it never occurred to either of them that the answers to their questions
might be the same. Their knowledge blinded them from seeing the
commonalities. This sort of tunnel vision is fairly common and part of
the reason why sharing research is so encouraged within the scientific
community.
Similarly, for a laymen, the dramatic differences between these two types of
branes are less clear. Just as someone who doesn't study much religion may
be confused by the difference between Episcopalian and Catholic theological
doctrines, to a priest of either religion the differences are well-known, and
the two are seen as extremely distinct.
In the case of branes, though, the laymen would have had clearer insight
on the issue than either of the experts. The very details that made D-branes
and p-branes so intriguing to Polchinski and Strominger hindered their
ability to see past the details to the commonalities — at least until 1995,
when Polchinski finally saw the connection.
Because of equivalence, both D-branes and p-branes are typically just referred
to as branes. When referencing their dimensionality, the p-brane notation is
usually the one used. Some physicists still use the D-brane notation because
there are other types of branes that physicists talk about. (For the remainder
of this book, I mainly refer to them as branes, thus saving wear and tear on my
keyboard's D key.)
Using branes to explain black holes
One of the major theoretical insights that string theory has offered is the
ability to understand some black hole physics. These are directly related to
work on p-branes, which, in certain configurations, can act something like
black holes.
The connection between branes and black holes was discovered by Andrew
Strominger and Cumrun Vafa in 1996. This is one of the few aspects of string
theory that can be cited as actively confirming the theory in a testable way,
so it's rather important.
The starting point is similar to Strominger's work on p-branes to create
particles: Consider a tightly curled region of a space-dimension that has a
brane wrapped around it. In this case, though, you're considering a situation
in which gravity doesn't exist, which means you can wrap multiple branes
around the space.
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together / yj
The brane's mass limits the amount of electromagnetic charge the brane can
contain. A similar phenomenon happens with electromagnetically charged
black holes. These charges create an energy density, which contributes to the
mass of the black hole. This places a limit on the amount of electromagnetic
charge a stable black hole can contain.
In the case where the brane has the maximum amount of charge — called an
extremal configuration — and the case where the black hole has the maximum
amount of charge — called an extremal black hole — the two cases share
some properties. This allows scientists to use a thermodynamic model of an
extremal configuration brane wrapped around extra dimensions to extract
the thermodynamic properties that scientists would expect to obtain from an
extremal black hole. Also, you can use these models to relate near-extremal
configurations with near-extremal black holes.
Black holes are one of the mysteries of the universe that physicists would
most like to have a clear explanation for. For more details on how string
theory relates to black holes, skip ahead to Chapter 14.
String theory wasn't built with the intention of designing this relationship
between wrapped branes and black holes. The fact that an artifact extracted
purely from the mathematics of string theory would correlate so precisely
with a known scientific object like a black hole, and one that scientists
specifically want to study in new ways, was seen by everyone as a major
step in support of string theory. It's just too perfect, many think, to be mere
coincidence.
Getting stuck on a brane: Brane Worlds
With the introduction of all of these new objects, string theorists have begun
exploring what they mean. One major step is the introduction of brane world
scenarios, where our 3-dimensional universe is actually a 3-brane.
Ever since the inception of string theory, one of the major conceptual hurdles
has been the addition of extra dimensions. These extra dimensions are
required so the theory is consistent, but we certainly don't seem to experience
more than three space dimensions. The typical explanation has been to
compactify the extra six dimensions into a tightly wound object roughly the
size of the Planck length.
In the brane world scenarios, the reason we perceive only three spatial
dimensions is that we live inside a 3-brane. There's a fundamental difference
between the space dimensions on the brane and those off the brane.
196
Part III: Building String Theory: A Theory of Everything _
The brane world scenarios are a fascinating addition to the possibilities of
string theory, in part because they may offer some ways in which we can
have consistent string theories without resorting to elaborate compactification
scenarios. Not everyone is convinced, however, that compactifications can
be eliminated from the theory and even some brane world theories include
compactification as well.
In the "Infinite dimensions: Randall-Sundrum models" section later in this
chapter, I look at some specific brane world scenarios that have been proposed,
which offer some intriguing explanations for aspects of our universe, such as
how to resolve the hierarchy problem (from Chapter 8). In Chapter 15, the
idea of brane worlds allows you to consider the possibility of escaping our
universe and traveling to a different universe on another brane!
Matrix Theory as a Potential M-Theory
A year after the proposal of M-theory, Leonard Susskind introduced a
suggestion for what the "M" could stand for. Matrix theory proposes that the
fundamental units of the universe are O-dimensional point particles, which
Susskind calls partons (or DO-branes). (No, these particles have nothing to
do with the buxom Miss Dolly Parton.) These partons can assemble into
all kinds of objects, creating the strings and branes required for M-theory.
In fact, most string theorists believe that matrix theory is equivalent to
M-theory.
Matrix theory was developed by Leonard Susskind, Tom Banks, Willy
Fischler, and Steve Shenker in the year after Witten proposed M-theory.
(The paper on the topic wasn't published until 1997, but Susskind presented
the concept at a 1996 string theory conference prior to publication.) The
theory is also approximated by 11-dimensional supergravity, which is one
of the reasons string theorists think it's appropriate to consider it equal to
M-theory.
The name "parton," which Susskind uses in his book The Cosmic Landscape
(and I've used here) to describe these O-dimensional branes, comes from a
term used by the Nobel Prize-winning quantum physicist (and string theory
skeptic) Richard P. Feynman. Both Feynman and his colleague and rival
Murray Gell-Mann were working to figure out what made up hadrons. Though
Gell-Mann proposed the quark model, Feynman had described a more vague
theory where hadrons were made up of smaller pieces that he just called
partons.
One intriguing aspect of the partons, noted by Witten, is that as they get
close to each other, it becomes impossible to tell where the partons
actually are. This may be reminiscent of the uncertainty principle in quantum
mechanics, in which the position of a particle can't be determined with
absolute precision, even mathematically (let alone experimentally). It's
Chapter 11: M-Theory and Beyond: Bringing String Theory Together I y/
impossible to test this the same way scientists can test the uncertainty
principle, because there's no way to isolate and observe an individual parton.
Even light itself would be made up of a vast number of partons, so "looking"
at a parton is impossible.
Unfortunately, the mathematics involved in analyzing matrix theory is
difficult, even by the standards string theorists use. For now, research
continues, and string theorists are hopeful that new insights may show
more clearly how matrix theory can help shed light on the underlying
structure of M-theory.
Gaining Insight from the
Holographic Principle
Another key insight into string theory comes from the holographic principle,
which relates a theory in space to a theory defined only on the boundary of
that space. The holographic principle isn't strictly an aspect of string theory
(or M-theory), but applies more generally to theories about gravity in any
sort of space. Because string theory is such a theory, some physicists believe
the holographic principle will lie at the heart of it.
Capturing multidimensional information
on a flat surface
It turns out, as shown by Gerard 't Hooft in 1993 (and developed with much
help from Leonard Susskind), the amount of "information" a space contains
may be related to the area of a region's boundary, not its volume. (In quantum
field theory, everything can be viewed as information.) In short, the
holographic principle amounts to the following two postulates:
u* A gravitational theory describing a region of space is equivalent to a
I theory defined only on the surface area that encloses the region.
J-" The boundary of a region of space contains at most one piece of
information per square Planck length.
In other words, the holographic principle says that everything that happens
in a space can be explained in terms of information that's somehow stored
on the surface of that space. For example, picture a 3-dimensional space that
resides inside the 2-dimensional curled surface of a cylinder, as in Figure 11-2.
You reside inside this space, but perhaps some sort of shadow or reflection
resides on the surface.
/ yO Part III: Building String Theory: A Theory of Everything _
Now, here's a key aspect of this situation that's missing from our example: A
shadow contains only your outline, but in 't Hooft's holographic principle, all
of the information is retained. (See the nearby sidebar, "Inside a hologram.")
Another example, and one that is perhaps clearer, is to picture yourself
inside a large cube. Each wall of the cube is a giant television screen, which
contains images of the objects inside the cube. You could use the informa-
tion contained on the 2-dimensional surface of the space to reconstruct the
objects within the space.
Again, though, this example falls short because not all of the information is
encoded. If I were to have objects blocking me in all six directions, my image
wouldn't be on any of the screens. But in the holographic principle view of
the universe, the information on the surface contains all the information that
exists within the space.
Connecting the holographic
principle to our reality
The holographic principle is totally unexpected. You'd think that the informa-
tion needed to describe a space would be proportional to the volume of that
space. (Note that in the case of more than three space dimensions, "volume"
isn't a precise term. A 4-dimensional "hypervolume" would be length times
width times height times some other space direction. For now, you can
ignore the time dimension.)
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together 1 yy
Inside a hologram
A hologram is a 2-dimensional image that
contains all the 3-dimensional information of an
object. When viewing a hologram, you can tilt
the image and see the orientation of the shape
move. It's as if you see the object in the picture
from a different angle. The process of making a
hologram is called holography.
This is achieved through the interference
patterns in light waves. The process involves
using a laser — so all of the light has exactly
the same wavelength — and reflecting it off of
the object onto a film. (When I performed this
experiment in my college Optics class, I used a
small plastic horse.)
As the light strikes the film, it records
interference patterns that, when properly
developed, allow the film to encode the
information about the 3-dimensional shape that
was holographed. The encoded information
then has to be decoded, which means the laser
light again has to be shown through the film in
order to see the image.
"White light" holograms exist, which don't
need laser light to view them. These are the
holograms that you're most familiar with, which
manifest their image in ordinary light.
You can consider this principle in two ways:
13 f Our universe is a 4-dimensional space that is equivalent to some
I 3-dimensional boundary.
v* Our universe is a 4-dimensional boundary of a 5-dimensional space,
which contains the same information.
In scenario 1, we live in the space inside the boundary, and in scenario 2,
we are on the boundary, reflecting a higher order of reality that we don't
perceive directly. Both theories have profound implications about the nature
of the universe we live in.
Considering AdS/CFT correspondence
Though presented in 1993, even Leonard Susskind says he thought it would
be decades before there would be any way to confirm the holographic
principle. Then, in 1997, Argentinean physicist Juan Maldacena published a
paper, inspired by the holographic principle, that proposed something
called the anti-de Sitter/conformal field theory correspondence, or AdS/CFT
correspondence, which brought the holographic principle to center stage in
string theory.
2(/(/ P art '" : Building String Theory: A Theory of Everything _
In Maldacena's AdS/CFT correspondence, he proposed a new duality
between a gauge theory defined on a 4-dimensional boundary (three space
dimensions and one time dimension) and a 5-dimensional region (four space
dimensions and one time dimension). In essence, he showed that there are
circumstances in which the holographic principle scenario 2 is possible (see
the preceding section).
As usual in string theory, one of those conditions is unbroken supersymmetry.
In fact, the theoretical world he studied had the most amount of supersymmetry
possible — it was maximally supersymmetrical.
Another condition was that the 5-dimensional region was something called
an anti-de Sitter space, which means it had negative curvature. Our universe
(at least at present) is more similar to a de Sitter space, as mentioned in
Chapter 9. As such, it hasn't yet been proved that the AdS/CFT correspondence
(or something similar) specifically applies to our own universe (though
thousands of papers have been written on the subject).
Even if the duality turns out not to be completely true, a growing body of
theoretical work supports the idea that there is some sort of correspondence
between string theory and gauge theory, even if only at some low levels of
approximation. Calculations that are hard in one version of the theory may
actually be easy in the other one, meaning that it may be crucial in figuring
out how to complete the theory. This has helped support the idea that the
holographic principle may ultimately prove to be one of the fundamental
principles of M-theory.
The holographic principle, and specifically the AdS/CFT correspondence,
may also help scientists further understand the nature of black holes. The
entropy (or disorder) of a black hole is proportional to the surface area of
the black hole, not its volume. This is one of the arguments in support of
the holographic principle, because it's believed that it would offer further
physical explanation of black holes.
String Theory Gets Surprised
by bark Energy
The discovery of dark energy in 1998 meant that our universe needed to
have a positive cosmological constant. The problem is that all of the string
theories were built in universes with negative cosmological constants (or a
zero value). When work did discover possible ways to incorporate a positive
cosmological constant, it resulted in a theory that has a vast number of
possibilities!
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together «£ (J /
Dark energy is an energy that seems to fill much of the universe and causes
space-time to expand. By current estimates, more than 70 percent of the
universe is comprised of dark energy.
Prior to the 1998 discovery, the assumption was that the universe had a zero
cosmological constant, so all the work done in string theory was focused on
that sort of a universe. With the discovery of dark matter, priorities had to
change. The search was on for a universe that had a positive cosmological
constant.
Joe Polchinski and Raphael Bousso extended others' earlier research by
experimenting with extra dimensions that had electric flux (a number that
represents the intensity of an electric field through a surface) wrapped
around them. Branes carried charge, so they could also have flux. This
construction had the potential to limit some parameters of the theory in a
way that couldn't vary continuously.
In 2003, a Stanford group including Renata Kallosh, Andrei Linde, Shamit
Kachru, and Sandip Trivedi released a paper that showed ways to extend
the Polchinski-Bousso thinking to construct string theories with a positive
cosmological constant. The trick was to create a universe and then wrap it
with branes and anti-branes to contain the electric and magnetic flux. This
introduced the potential for two effects:
J-" It allowed a small positive cosmological constant,
v" It stabilized the extra dimensions in string theory.
On the surface, this would seem to be an excellent outcome, providing two
necessary components to string theory. Unfortunately, there was one little
problem — there were far too many solutions!
Considering Proposals for Why
Dimensions Sometimes Uncurl
Most string theory proposals have been based on the concept that the extra
dimensions required by the theory are curled up so small that they can't be
observed. With M-theory and brane worlds, it may be possible to overcome
this restriction.
A few scenarios have been proposed to try to describe a mathematically
coherent version of M-theory, which would allow the extra dimensions to be
extended. If any of these scenarios hold true, they have profound implications
for how (and where) physicists should be looking for the extra dimensions of
string theory.
2(/2 P art '" : Building String Theory: A Theory of Everything
Measurable dimensions
One model that has gotten quite a bit of attention was proposed in 1998 by
Savas Dimopoulos, Nima Arkani-Hamed, and Gia Dvali. In this theory, some of
the extra dimensions could be as large as a millimeter without contradicting
known experiments, which means that it may be possible to observe their
effects in experiments conducted at CERN's Large Hadron Collider (LHC).
(This proposal has no unique name, but I call it MDM for millimeter dimension
model. Who knows, maybe it'll catch on!)
When Dimopoulos introduced MDM at a 1998 supersymmetry conference, it
was actually something of a subversive act. He was making a bold statement:
Extra dimensions were as important, if not more so, than supersymmetry.
Many physicists believe that supersymmetry is the key physical principle
that will prove to be the foundation of M-theory. Dimopoulos proposed that
the extra dimensions — previously viewed as an unfortunate mathematical
complication to be ignored as much as possible — could be the fundamental
physical principle M-theory was looking for.
In MDM, a pair of extra dimensions could extend as far as a millimeter away
from the 3-dimensional brane that we reside on. If they extend much more than
a millimeter, someone would have noticed by now, but at a millimeter, the
deviation from Newton's law of gravity would be so slight that no one would
be any the wiser. So because gravity is radiating out into extra dimensions, it
would explain why gravity is so much weaker than the brane-bound forces.
The way this works is everything in our universe is trapped on our 3-
dimensional brane except gravity, which can extend off of our brane to affect
the other dimensions. Unlike in string theory, the extra dimensions wouldn't
be noticeable in experiments except for gravity probes, and in 1998, gravity
hadn't been tested at distances shorter than a millimeter.
Now, don't get too excited yet. Experiments have been done to look for these
extra millimeter-sized dimensions and, it turns out, they probably don't exist.
Experiments show that the dimensions have to be at least as small as a tenth
of a millimeter, but that's still far larger than in most other string theory
scenarios. Instead of requiring the 10 19 GeV (giga-electronvolts, a unit of
energy) needed to explore the Planck length, exploring a millimeter would
require only 1,000 GeV — still within the range of CERN's LHC!
Infinite dimensions: Randatt-Sundmm models
If a millimeter-sized dimension turned heads, the 1999 proposal by Lisa
Randall and Raman Sundrum was even more spectacular. In these Randall-
Sundrum models, gravity behaves differently in different dimensions,
depending on the geometry of the branes.
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together 20 J
Yet another string theory: F-theory
Another theory that sometimes gets discussed
is called F-theory (the name is a joking
reference to the idea that the M in M-theory
stands for mother). Cumrun Vafa proposed
F-theory in 1996 after noticing that certain
complicated solutions of Type MB string theory
could be described in terms of a simpler
solution of a differenttheory with 12 dimensions,
up from the 10 dimensions of superstrings or the
11 dimensions of M-theory. Unlike M-theory,
where all the dimensions of space-time are
treated on equal footing, two of the dimensions
of F-theory are fundamentally differentthan the
rest: They always have to be curled up. So now
to get to three space dimensions, we have eight
small dimensions instead of six!
This makes it seem as though the theory is
getting more complicated, but in fact the
F-theory description is often simpler. These
eight dimensions include not only all the
information from the previous six, but also infor-
mation about what branes exist in the solution
(those setups could get complicated). This is
an example of a common theme in the develop-
ment of string theory; more and more of the the-
ory's details, such as what particles exist and
how they interact, or what branes live where,
can be described simply in terms of the geom-
etry of the extra dimensions. This geometry is
often easier to understand and analyze.
F-theory has been receiving more attention in
the past few years because its rich structure
allows solutions that reproduce many of the
phenomena of the Standard Model and GUT
theories (see Chapter 12 for more on those).
In the original Randall-Sundrum model, called RSI, they propose a brane
that sets the strength of gravity. In this gravity brane, the strength of gravity
is extremely large. As you move in a fifth dimension away from the gravity-
brane, the strength of gravity drops exponentially.
An important aspect of the RSI model is that the strength of gravity depends
only on the position within the fifth dimension. Because our entire 3-brane
(this is a brane world scenario, where we're trapped on a 3-brane of space) is
at the same fifth-dimensional position, gravity is consistent everywhere in the
3-brane.
In a second scenario, called RS2, Randall and Sundrum realized that the
3-brane that we're stuck in could have its own gravitational influence. Though
gravitons can drift away from the 3-brane into other dimensions, they can't
get very far because of the pull of our 3-brane. Even with large dimensions,
the effects of gravity leaking into other dimensions would be incredibly small.
Randall and Sundrum called the RS2 model localized gravity.
In both of these models, the key feature is that gravity on our own 3-brane is
essentially always the same. If this weren't the case, we'd have noticed the
extra dimensions before now.
In 2000, Lisa Randall proposed another model with Andreas Karch called
locally localized gravity. In this model, the extra dimension contained some
201} P art '" : Building String Theory: A Theory of Everything _
negative vacuum energy. It goes beyond the earlier models, because it allows
gravity to be localized in different ways in different regions. Our local area
looks 4-dimensional and has 4-dimensional gravity, but other regions of the
universe might follow different laws.
Understanding the Current Landscape:
A Multitude of Theories
As far back as 1986, Andrew Strominger found that there was a vast number
of consistent string theory solutions and observed that all predictive power
may have been lost. Actually, when considering a negative cosmological
constant (or zero), you apparently end up with an infinite number of possible
theories.
With a positive cosmological constant — as needed in our universe, thanks
to dark energy — things get better, but not by much. There are now a finite
number of ways to roll up the branes and anti-branes so as to obtain a positive
cosmological constant. How many ways? Some estimates have indicated as
many as 10 500 possible ways to construct such a string theory!
This is an enormous problem if the goal of string theory was to develop a
single unified theory. The vision of both the first and second superstring
revolutions (or at least the vision guiding some bandwagoners who jumped
on board) was a theory that would describe our universe with no
experimental observations required.
In 2003, Leonard Susskind published "The Anthropic Landscape of String
Theory," in which he very publicly gave up the idea that a unique string
theory would be discovered. In the paper, Susskind introduced the concept
of "the landscape" of string theories: a vast number of mathematically
consistent possible universes, some of which actually exist. Susskind's string
theory landscape was his solution to the unfathomable number of possible
string theories.
But with so many possibilities, does the theory have any predictive power?
Can we use a theory if we don't know what the theory is?
The anthropic principle requires observers
Susskind's proposed solution involves relying on something known as the
anthropic principle. This principle indicates that the reason the universe has
the properties it does is because we're here to observe them. If it had vastly
different properties, we wouldn't exist. Other areas of the multiverse may
have different properties, but they're too far away for us to see.
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together 2(/3
111% 1 ^ ne antnro Pi c principle was coined by Cambridge astrophysicist Brandon
SBSI I Carter in 1974. It exists in two basic versions:
v* Weak anthropic principle: Our location (or region) of space-time
possesses laws such that we exist in it as observers.
J-" Strong anthropic principle: The universe is such that there has to exist
a region of space-time within it that allows observers.
If you're reading these two variations of the anthropic principle and scratching
your head, you're in good company. Even string theorists who are now
embracing the anthropic principle — such as Susskind and Joe Polchinski —
once despised it as totally unscientific. This is in part due to the fact that the
anthropic principle (in its strong form) is sometimes invoked to require a
supernatural designer of the universe, something that most scientists (even
religious ones) try to avoid in their scientific work. (Ironically, it is also often
used, in the weak form, as an argument against a supernatural designer, as
Susskind does in his book The Cosmic Landscape?)
For the anthropic principle to make sense, you have to consider an array of
possible universes. Figure 11-3 shows a picture of the energy levels of possible
universes, where each valley represents a particular set of string theory
parameters.
You are
here
206
Part III: Building String Theory: A Theory of Everything _
According to the weak anthropic principle, the only portions of the multiverse
we can ever observe are the ones where these parameters allow us to exist.
In this sense, the weak anthropic principle is almost a given — it's just always
going to be true. That's part of the point of it. Because we're here, we can
use the fact that we're here to explain the properties the universe has. In
the string theory landscape, so many possibilities are out there that ours is
just one of them, which has happened to come into being, and we're lucky
enough to be here.
^VftBEfl If the string theory landscape represents all the universes that are possible,
' Y w\ the multiverse represents all the universes that actually exist. Distant regions
|M|| J of the multiverse may have radically different physical properties than those
that we observe in our own section.
This concept is similar to Lisa Randall's locally localized gravity (see the
"Infinite dimensions: Randall-Sundrum models" section earlier in this chapter),
where only our local region exhibits the gravity that we know and love in
three space dimensions. Other regions could have five or six space dimensions,
but that doesn't matter to us, because they're so far away that we can't see
them. These other regions are different parts of the multiverse.
In 1987, Nobel Prize-winner Steven Weinberg added a bit of credibility to the
field. Using reasoning based on the anthropic principle, he analyzed the
cosmological constant required to create a universe like ours. His prediction
was a very small positive cosmological constant, only about one order of
magnitude off from the value found more than a decade later.
This is a frequently cited case of when the anthropic principle led to a
testable prediction, but I've never been particularly convinced that it's that
meaningful. Clearly, our universe is one in which galaxies formed the way
they have — not too fast or too slow. Using that fact is totally uncontroversial
as a means of determining the cosmological constant, but the anthropic
principle goes further. It doesn't just determine the cosmological constant, it
supposedly explains why the cosmological constant has that value.
The key feature of anthropic reasoning is that there exists an entire multiverse
of possibilities. If there's just one universe, we have to explain why that universe
is so perfectly suited for humans to exist. But if there are a vast number of
universes, and they take on a wide range of parameters, then probability
dictates that every once in a while a universe like ours will spring up, resulting
in life forms and observers like us.
_Chapter 11: M-Theory and Beyond: Bringing String Theory Together 20/
Disagreeing about the principle's Value
Since its introduction in 1974, the anthropic principle has invoked passion
among scientists. It's safe to say that most physicists don't consider invoking
the anthropic principle to be the best scientific tactic. Many physicists see it
as giving up on an explanation, and just saying "it is what it is."
At Stanford, Leonard Susskind and his colleagues seem to be embracing the
anthropic principle. To hear (or read) Susskind on the subject, the string
theory community is quickly jumping on board. It's unclear whether the
movement is spreading quite as intently as this rhetoric implies, though.
One barometer could be the literature. Out of 13 string theory books (written
after 2003 — 8 popular books, 5 textbooks) within my reach at this moment,
here are the statistics:
v" 5 make no mention of the anthropic principle in the index
v" 2 discuss the anthropic principle for precisely one paragraph
J-" 2 contain more general discussions of the anthropic principle, lasting
about two pages
J-" 2 attack the landscape and anthropic principle as major failures of the
theory, devoting roughly an entire chapter to the concept
(-" 2 argue that the anthropic principle is crucial to understanding our
universe (and one of those is written by Susskind himself)
On the other hand, a search of the arXiv.org theoretical physics database
shows 218 hits on a search of the phrase "anthropic." Searching on
"anthropic principle" obtains 104 hits, and adding words such as "string"
and "brane" only causes it to drop from there. For comparison, searching on
"string theory," "cosmological constant," or even the far less popular "loop
quantum gravity" result in so many hits that the search cuts off at only 1,000
papers. So the jury is certainly still out on how well the string theory
community has adopted the anthropic principle.
Some string theorists, such as David Gross, appear to be strongly opposed to
anything that even hints at the anthropic principle. A large number of string
theorists bought into it based on the idea — championed by Witten's
promise of M-theory in 1995 — that there would be a single theory at the end
of the rainbow.
2(/0 P art '" : Building String Theory: A Theory of Everything _
String theorists seem to be turning to the anthropic principle mostly out of a
lack of other options. This certainly seems to be the case for Edward Witten,
who has made public statements indicating he might be unenthusiastically
turning toward anthropic thinking.
We end the chapter in many ways worse off than we began. Instead of five
distinct string theory solutions, we have 10 500 or so. It's unclear what the
fundamental physical properties of string theory are in a field of so many
options. The only hope is that new observations or experiments will provide
some sort of clue about which aspect of the string theory landscape to
explore next.
Chapter 12
Putting String Theory to the Test
In This Chapter
Picking the right string theory to test
Disproving string theory may be harder than confirming it
Exploring two types of labs: Nature's lab and particle accelerators
J\]o matter how impressive string theory is, without experimental
W w confirmation, it's nothing but mathematical speculation. As discussed
in Chapter 4, science is an interplay of theory and experiment. String theory
attempts to structure the experimental evidence around a new theoretical
framework.
One problem with string theory is that the energy required to get direct
evidence for the distinct predictions of the theory is typically so high that it's
very hard to reach. New experimental methods, such as the Large Hadron
Collider (described later in this chapter), are expanding our ability to test in
higher energy ranges, possibly leading to discoveries that more strongly
support string theory predictions, such as extra dimensions and super-
symmetry. Probing the strings themselves requires massive amounts of
energy that are still far away from any experimental exploration.
In this chapter, my goal is to look at different ways that string theory can
be tested, so it can be either verified or disproved. First, I explain the work
that still needs to be done to complete the theory so it can make meaningful
predictions. I also cover a number of experimental discoveries that would
pose complications for string theory. Then I discuss ways of proving that our
universe does contain supersymmetry, a key assumption required by string
theory. Finally, I outline the testing apparatus — those created in deep space
and particle accelerators created on Earth.
2 1 (/ P ar t HI: Building String Theory: A Theory of Everything _
Understanding the Obstacles
&SL
As discussed in Chapter 11, string theory isn't complete. There are a vast
number of different string theory solutions — literally billions of billions of
billions of billions of different possible variants of string theory, depending on
the parameters introduced into the theory. So, in order to test string theory,
scientists have to figure out which predictions the theory actually makes.
Before testing on string theory can take place, physicists need to filter
through the massive possible number of solutions to find a manageable
amount that may describe our universe. Most of the current tests related to
string theory are measurements that are helping to define the current
parameters of the theory. Then, after the remaining theoretical solutions
are somehow assessed in a reasonable way, scientists can begin testing the
unique predictions they make.
There are two features common to (almost) all versions of string theory, and
scientists who are looking for evidence of string theory are testing these ideas
even now:
(-" Supersymmetry
w Extra dimensions
These are string theory's two cornerstone ideas (aside from the existence of
strings themselves, of course), which have been around since the theory was
reformulated into superstring theory in the 1970s. No theory that has tried to
eliminate them has lasted very long.
Testing an incomplete theory
With indistinct predictions
Right now, there is a great deal of confusion over what physical properties
(other than supersymmetry and extra dimensions) lie at the heart of string
theory. The holographic principle, anthropic principle, brane world scenarios,
and other such approaches are becoming more popular, but scientists don't
know for certain how they apply in the case of our universe.
The energy constraints on string theory experiments are obviously a big
obstacle, but I think for most skeptical theorists, lack of specific, distinct
experiments is the more disturbing issue. The variants of string theory make
few distinct predictions, so it's hard to even think about testing it. Scientists
can continue to test aspects of the Standard Model, to make sure that string
.Chapter 12: Putting String Theory to the Test 211
theory predictions remain consistent, and they can look for properties such
as supersymmetry or extra dimensions, but these are very general predictions,
many of which are made not just by string theory. The first step in testing
string theory is to figure out what the theory is telling us that is distinct from
other theories.
Test Versus proof
There's really no way to prove something like string theory, as a whole. You
can prove that a specific prediction (such as supersymmetry, which I get
to later in this chapter) is true, but that doesn't prove that the theory as a
whole is true. In a very real sense, string theory can never be proved; it can
just meet the test of time, the same way that other theories have done.
For scientists, this slight distinction is known and accepted, but there's some
confusion about it among nonscientists. Most people believe that science
proves things about the laws of nature beyond a shadow of a doubt, but
the truth is that science dictates there is always a shadow of a doubt in any
theory.
A theory can be tested in two ways. The first is to apply the theory to explain
existing data (called apostdictiori). The second is to apply the theory to
determine new data, which experiments can then look for. String theory has
been very successful at coming up with postdictions, but it hasn't been as
successful at making clear predictions.
String theory, as Chapter 17 explains, has some valid criticisms that need to
be addressed. Even if they are addressed, string theory will never be proved,
but the longer it makes predictions that match experiments, the more support
it will gain.
For this to happen, of course, string theory has to start making predictions
that can be tested.
Testing Supersymmetry
One major prediction of string theory is that a fundamental symmetry exists
between bosons and fermions, called supersymmetry. For each boson there
exists a related fermion, and for each fermion there exists a related boson.
(Bosons and fermions are types of particles with different spins; Chapter 8
has more detail about these particles.)
jt 7 4m ' >art '" : Building String Theory: A Theory of Everything _
Finding the missing spartictes
Under supersymmetry, each particle has a superpartner. Every boson has a
corresponding fermionic superpartner, just as every fermion has a bosonic
superpartner. The naming convention is that fermionic superpartners end
in "-ino," while bosonic superpartners start with an "s." Finding these
superpartners is a major goal of modern high-energy physics.
The problem is that without a complete version of string theory, string
theorists don't know what energy levels to look at. Scientists will have to
keep exploring until they find superpartners and then work backward to
construct a theory that contains the superpartners. This seems only slightly
better than the Standard Model of particle physics, where the properties of
all 18 fundamental particles have to be entered by hand.
Also, there doesn't appear to be any fundamental theoretical reason why
scientists haven't found superpartners yet. If supersymmetry does unify the
forces of physics and solve the hierarchy problem, then scientists would
expect to find low-energy superpartners. (The search for the Higgs boson
has undergone these same issues within the Standard Model framework for
years. It has yet to be detected experimentally either.)
Instead, scientists have explored energy ranges into a few hundred GeV, but
still haven't found any superpartners. So the lightest superpartner would
appear to be heavier than the 17 observed fundamental particles. Some
theoretical models predict that the superpartners could be 1,000 times
heavier than protons, so their absence is understandable (heavier particles
often tend to be more unstable and collapse into lower-energy particles if
possible) but still frustrating.
Right now, the best candidate for a way to find supersymmetric particles
outside of a high-energy particle accelerator (see the later section "Large
Hadron Collider (LHC)") is the idea that the dark matter in our universe may
actually be the missing superpartners (see the later section "Analyzing dark
matter and dark energy").
Testing implications of supersymmetry
If supersymmetry exists, then some physical process takes place that causes
the symmetry to become spontaneously broken as the universe goes from
a dense high-energy state into its current low-energy state. In other words,
as the universe cooled down, the superpartners had to somehow decay
into the particles we observe today. If theorists can model this spontaneous
symmetry-breaking process in a way that works, it may yield some testable
predictions.
.Chapter 12: Putting String Theory to the Test 213
The main problem is something called the flavor problem. In the standard
model, there are three flavors (or generations) of particles. Electrons, muons,
and taus are three different flavors of leptons.
In the Standard Model, these particles don't directly interact with each
other. (They can exchange a gauge boson, so there's an indirect interaction.)
Physicists assign each particle numbers based on its flavor, and these numbers
are a conserved quantity in quantum physics. The electron number, muon
number, and tau numbers don't change, in total, during an interaction. An
electron, for example, gets a positive electron number but gets for both
muon and tau numbers.
Because of this, a muon (which has a positive muon number but an electron
number of zero) can never decay into an electron (with a positive electron
number but a muon number of zero), or vice versa. In the Standard Model and
in supersymmetry, these numbers are conserved, and interactions between
the different flavors of particles are prohibited.
However, our universe doesn't have supersymmetry — it has broken
supersymmetry. There is no guarantee that the broken supersymmetry
will conserve the muon and electron number, and creating a theory of
spontaneous supersymmetry breaking that keeps this conservation intact is
actually very hard. Succeeding at it may provide a testable hypothesis,
allowing for experimental support of string theory.
Testing Gravity from Extra Dimensions
The testing of gravity produces a number of ways to see if string theory
predictions are true. When physicists test for gravity outside of our three
dimensions, they
K" Search for a violation of the inverse square law of gravity
If-" Search for certain signatures of gravity waves in the cosmic microwave
background radiation (CMBR)
It may be possible that further research will result in other ways to determine
the behavior of string theory or related concepts (see the nearby sidebar,
"Detecting the holographic principle with gravity waves").
211) P art l" : Building String Theory: A Theory of Everything
Testing the inverse square taW
If extra dimensions are compactified in ways that string theorists have typically
treated them, then there are implications for the behavior of gravity.
Specifically, there might be a violation of the inverse square law of gravity,
especially if gravitational force extends into these extra dimensions at small
scales. Current experiments seek to test gravity to an unprecedented level,
hoping to see these sorts of differences from the established law.
The behavior of gravity has been tested down to under a millimeter, so any
compactified dimensions must be smaller than that. Recent models indicate
that they may be as large as that, so scientists want to know if the law of
gravitation breaks down around that level.
As of this book's publication, no evidence has been found to confirm the
extra dimensions at this level, but only time will tell.
Searching for gravity vOaVes in the CMBR
General relativity predicts that gravity moves in waves through space-time.
Although string theory agrees with this prediction, in most string theory-
based models of inflation, there are no observable gravity waves in the
cosmic microwave background radiation (CMBR). Traditional inflation
models that don't take string theory into account do predict CMBR gravity
waves.
Again, this turns out to be a search for evidence against string theory, but
this has a bit more weight behind it than some of the others. Although the
string theory landscape has predictions for scenarios where relativity breaks
down, there doesn't appear to be any mechanism in string theory for gravity
waves in the CMBR, according to University of California cosmologist and
string theorist Andrei Linde. (Linde made this statement in 2007 and work
since then has produced some preliminary indications that string theory
models of inflation may be compatible with gravity waves in the CMBR.)
At present, the evidence seems to be leaning toward there not being any
gravity waves in the CMBR data. The Planck Surveyor spacecraft was
successfully launched in May 2009, with even greater sensitivity than the
current WMAP study. Scientists may get a more decisive take on whether
these CMBR gravity waves exist at any time.
.Chapter 12: Putting String Theory to the Test 215
Detecting the holographic principle
with gravity waves
Results from the GE0600 gravity wave detector
in Germany may already have found evidence
for the holographic principle, though the co-
creator of the holographic principle is skeptical.
In 2007, Fermilab physicist Craig Hogan realized
that if the bits of information on the surface
of space are Planck length in size (as the
holographic principle suggests), the bits of
information contained inside the space have
to be larger. He then predicted that this would
cause some static in gravity wave detectors.
And, sure enough, static was being detected
by GE0600 in precisely the way predicted.
This would seem like an open and shut case,
but there are many possible sources of this
noise in the GE0600, and until they're eliminated
everyone is cautiously optimistic. Plus, Hogan's
paper is not so much a theory as a neat idea,
and no one is exactly sure what it means —
including string theory and holographic
principle co-founder Leonard Susskind.
Susskind told me in an e-mail that he doesn't
understand how the holographic principle
would result in gravitational wave noise.
Disproving String Theory
Sounds Easier Than It Is
With any theory, it's typically easier to disprove it than to prove it, although
one criticism of string theory is that it may have become so versatile that
it can't be disproved. I elaborate on this concern in Chapter 17, but in the
following sections I assume that string theorists can pull together a specific
theory. Having a working theory in hand makes it easier to see how it could
be proved wrong.
Violating relativity
String theories are constructed on a background of space-time coordinates,
so physicists assume relativity is part of the environment. If relativity turns
out to be in error, then physicists will need to revise this simplifying
assumption, although it's unlikely that this alone would be enough to cause
them to abandon string theory entirely (nor should it).
216
Part III: Building String Theory: A Theory of Everything _
There are theories that predict errors in relativity, most notably the variable
speed of light (VSL) cosmology theories of John Moffat, and Andreas Albrecht
and Joao Magueijo. Moffat went on to create a more comprehensive revision
of general relativity with his modified gravity (MOG) theories. These theories
are addressed in Chapter 19, but they mean that the current assumptions of
string theory contain errors.
Even in this case, though, string theory would survive. Elias Kiritsis and
Stephon Alexander have both proposed VSL theories within the context of
string theory. Alexander went on to do further work in this vein with the "bad
boy of cosmology," Joao Magueijo, who is fairly critical of string theory as a
whole.
Mathematical inconsistencies
Given that string theory exists only on paper right now, one major problem
would be a definitive proof that the theory contained mathematical
inconsistencies. This is the one area where string theory has proved most
adaptable, successfully avoiding inconsistencies for more than 20 years.
Of course, scientists know that string theory isn't the whole story — the true
theory is an 1 1-dimensional M-theory, which has not yet been defined. Work
continues on various string theory approximations, but the fundamental
theory — M-theory — may still prove to be nothing more than a myth (yet
another word the M could stand for).
One weakness is in the attempt to prove string theory finite. In Chapter 17,
you can read about the controversy over whether this has been achieved. (It
appears that even among string theorists there's a growing acknowledgement
that the theory hasn't been proved finite to the degree that it was once hoped
it would be.)
To create his theory of gravity, Newton had to develop calculus. To develop
general relativity, Einstein had to make use of differential geometry and
develop (with the help of his friend Marcel Grossman) tensor calculus.
Quantum physics was developed hand in hand with group representation
theory by innovative mathematician Hermann Weyl. (Group representation
theory is the mathematical study of how symmetries can act on vector
spaces, which is at the heart of modern physics.)
Though string theory had already spawned innovative mathematics
explorations, the fact that scientists don't have any complete version of
M-theory implies to some that some key mathematical insight is missing —
or that the theory simply doesn't exist.
.Chapter 12: Putting String Theory to the Test ^17
Could Proton Decay Spell Disaster)
If one of the older attempts at unification of forces (called grand unification
theories or GUTs) proves successful, it would have profound implications for
string theory. One of the most elegant GUTs was the 1974 Georgi-Glashow
model, proposed by Howard Georgi and Sheldon Glashow. This theory has
one flaw: It predicts that protons decay, and experiments over the last 25
years have not shown this to be the case. Even if proton decay is detected,
string theorists may be able to save their theory.
The Georgi-Glashow model allows quarks to transform into electrons and
neutrinos. Because protons are made of specific configurations of quarks, if
a quark inside a proton were to suddenly change into an electron, the proton
itself would cease to exist as a proton. The nucleus would emit a new form of
radiation as the proton decayed.
^S-STo/^ This quark transformation (and resulting proton decay) exists because the
Georgi-Glashow model uses a SU(5) symmetry group. In this model, quarks,
electrons, and neutrinos are the same fundamental kind of particle, manifesting
in different forms. The nature of this symmetry is such that the particles can,
in theory, transform from one type into another.
Of course, these decays can't happen very often, because we need protons to
stick around if we're going to have a universe as we know it. The calculations
showed that a proton decays at a very small rate: less than one proton every
10 33 years.
This is a very small decay rate, but there's a way around it by having a lot
of particles. Scientists created vast tanks filled with ultrapure water and
shielded from cosmic rays that could interfere with protons (and give false
decay readings). They then waited to see if any of the protons decayed.
After 25 years, there has been no evidence of proton decay, and these
experiments are constructed so there could be as many as a few decays a
year. The results from the Super-Kamiokande, a neutrino observatory in
Japan, show that an average proton would take at least 10 35 years to decay.
To explain the lack of results, the Georgi-Glashow model has been modified
to include longer decay rates, but most physicists don't expect to observe
proton decay anytime soon (if at all).
If scientists did finally discover the decay of a proton, that would mean that
the Georgi-Glashow model would need to be looked at anew. String theory
gained success in part because of the failure of all other previous models, so
if their predictions work, it may indicate poor prospects for string theory.
2 1 P art '" : Building String Theory: A Theory of Everything _
The string theory landscape remains as resilient as ever, and some predictions
of string theory allow for versions that include proton decay. The decay
timeframe predicted is roughly 10 35 years — exactly the lower limit allowed
by the Super-Kamiokande neutrino observatory.
The renewal of GUTs would not disprove string theory, even though the
failure of GUT is part of the reason why string theory was originally adopted.
String theories can now incorporate GUT in low-energy domains. But string
theory can't tell us whether we should anticipate that GUT exists or protons
decay. Maybe or maybe not, and string theory can deal with it either way.
This is just one of the many cases where string theory shows a complete
ambivalence to experimental evidence, which some critics say makes it "un-
falsifiable" (as discussed at greater length in Chapter 17).
Looking for Evidence in the Cosmic
Laboratory: Exploring the Universe
The problem with conducting experiments in string theory is that it requires
massive amounts of energy to reach the level where the Standard Model
and general relativity break down. Although I address manmade attempts
to explore this realm in the next section, here I look at the different route
the field of string cosmology takes — attempting to look into nature's own
laboratory, the universe as a whole, to find the evidence that string theorists
need to test their theories.
Using outer space rays
to amplify small events
Among the various phenomena in the universe, two types produce large
amounts of energy and may provide some insight into string theory: gamma
ray bursts (GRBs) and cosmic rays.
Some physical events are hard to see because they
U* Are very rare (like, possibly, proton decay)
Iv Are very small (like Planck-scale events or possible deviations in
gravity's effects)
v" Happen only at very high energies (like high-energy particle collisions)
.Chapter 12: Putting String Theory to the Test 2 / y
Or, some combination of the three makes the event a challenge to witness.
Scientists are unlikely to see these improbable events in laboratories on
Earth, at least without a lot of work, so sometimes they look where they're
more likely to find them. Because both GRBs and cosmic rays contain very
high energies and take so long to reach us, scientists hope they can observe
these hard-to-see events by studying the cosmic happenings.
For years, physicists had used this method to explore potential breakdowns
in special relativity, but Italian physicist Giovanni Amelino-Camelia of the
University of Rome realized in the mid-1990s that this process could be used
to explore the Planck length (and energy) scale.
Gamma ray bursts
Exactly what causes a gamma ray burst is disputed, but it seems to happen
when massive objects, such as a pair of neutron stars or a neutron star and
a black hole (the most probable theories), collide with each other. These
objects orbit around each other for billions of years, but finally collapse
together, releasing energy in the most powerful events observed in the
universe, depicted in Figure 12-1.
The name gamma ray bursts clearly implies that most of this energy leaves
the event in the form of gamma rays, but not all of it does. These objects
release bursts of light across a range of different energies (or frequencies —
energy and frequency of photons are related).
220 P art '" : Building String Theory: A Theory of Everything _
According to Einstein, all the photons from a single burst should arrive at the
same time, because light (regardless of frequency or energy) travels at the
same speed. By studying GRBs, it may be possible to tell if this is true.
Calculations based on Amelino-Camelia's work has shown that photons of
different energy that have traveled for billions of years could, due to
(estimated and possibly over-optimistic) quantum gravity effects at the
Planck scale, have differences of about 1 one-thousandth of a second (0.001s).
The Fermi Gamma-ray Space Telescope (formerly the Gamma-ray Large Area
Space Telescope, or GLAST) was launched in June 2008 as a joint venture
between NASA, the U.S. Department of Energy, and French, German, Italian,
Japanese, and Swedish government agencies. Fermi is a low-Earth orbit
observatory with the precision required to detect differences this small.
So far, there's no evidence that Fermi has identified Planck scale breakdown
of general relativity. To date it's identified a dozen gamma ray-only pulsars, a
phenomenon that had never been observed before Fermi. (Prior to Fermi,
pulsars — spinning and highly magnetized neutron stars that emit energy
pulses — were believed to emit their energy primarily through radio waves.)
If Fermi (or some other means) does detect a Planck scale breakdown of
relativity, then that will only increase the need for a successful theory of
quantum gravity, because it will be the first experimental evidence that the
theory does break down at these scales. String theorists would then be able
to incorporate this knowledge into their theories and models, perhaps narrowing
the string theory landscape to regions that are more feasible to work with.
Cosmic rays
Cosmic rays are produced when particles are sent out by astrophysical
events to wander the universe alone, some traveling at close to the speed of
light. Some stay bound within the galactic magnetic field, while others break
free and travel between galaxies, traveling billions of years before colliding
with another particle. These cosmic rays can be more powerful than our
most advanced particle accelerators.
First of all, cosmic rays aren't really rays. They're stray particles in mostly
three forms: 90 percent free protons, 9 percent alpha particles (two protons
and two neutrons bound together — the nucleus of a helium atom), and 1
percent free electrons (beta minus particles, in physics-speak).
Astrophysical events — everything from solar flares to binary star collisions
to supernovae — regularly spit particles out into the vacuum of space, so our
planet (and, in turn, our bodies) are constantly bombarded with them. The
particles may travel throughout the galaxy, bound by the magnetic field of
the galaxy as a whole, until they collide with another particle. (Higher energy
particles, of course, may even escape the galaxy.)
.Chapter 12: Putting String Theory to the Test ££ /
Fortunately for us, the atmosphere and magnetic field of Earth protect us
from the most energetic of these particles so we aren't continuously dosed
with intense (and lethal) radiation. The energetic particles are deflected or
lose energy, sometimes colliding in the upper atmosphere to split apart into
smaller, less energetic particles. By the time they get to us, we're struck with
the less intense version of these rays and their offspring.
Cosmic rays have a long history as experimental surrogates. When Paul Dirac
predicted the existence of antimatter in the 1930s, no particle accelerators
could reach that energy level, so the experimental evidence of its existence
came from cosmic rays.
As the cosmic ray particles move through space, they interact with the
cosmic microwave background radiation (CMBR). This microwave energy
that permeates the universe is pretty weak, but for the cosmic ray particles,
moving at nearly the speed of light, the CMBR appears to be highly energetic.
(This is an effect of relativity, because energy is related to motion.)
In 1966, Soviet physicists Georgiy Zatsepin and Vadim Kuzmin, as well as the
independent work of Kenneth Greisen of Cornell University, revealed that
these collisions would have enough energy to create particles called mesons
(specifically called pi-mesons, or pions). The energy used to create the pions
had to come from somewhere (because of conservation of energy), so the
cosmic rays would lose energy. This placed an upper bound on how fast the
cosmic rays could, in principle, travel.
In fact, the GZK cutoff energy needed to create the pions would be about 10 19
eV (about one-billionth of the Planck energy of 10 19 GeV).
The problem is that, while most cosmic ray particles fall well below this
threshold, some very rare events that have had more energy than this
threshold — around 10 20 eV. The most famous of these observations was in
1991 at the University of Utah's Fly's Eye cosmic ray observatory on the U.S.
Army's Dugway Proving Ground.
Research since then indicates that the GZK cutoff does indeed exist. The rare
occurrence of particles above the cutoff is a reflection of the fact that, very
occasionally, these particles reach Earth before they come in contact with
enough CMBR photons to slow them down to the cutoff point.
These observations are in conflict with Japan's Akeno Giant Air Shower Array
(AGASA) project, which identified nearly ten times as many of these events.
The AGASA results implied a potential failure of the cutoff, which could
have had implications for a breakdown in relativity, but these other findings
decrease the probability of this explanation.
222 P art '" : Building String Theory: A Theory of Everything _
Still, the occasional existence of such energetic particles provides one means
of exploring these energy ranges, well above what current particle accelerators
could reach, so string theory may have a chance of an experimental test
using high-energy cosmic rays, even if they are incredibly rare.
Analyzing dark matter and dark energy
One other astronomical possibility to get results to support string theory
comes from the two major mysteries of the universe: dark matter and dark
energy. These concepts are discussed at length in Chapters 9 and 14.
The most obvious way that dark matter could help string theory is if it's
found that the dark matter is actually supersymmetric particles, such as the
photino (the superpartner of the photon) and other possible particles.
Another dark matter possibility is a theoretical particle called an axion,
originally developed outside of string theory as a means of conserving
certain symmetry relationships in quantum chromodynamics. Many string
theories contain the axion, so it could be a possibility as well, although the
properties suggested don't really match what cosmologists are looking for.
Some of the most significant work in cosmology and astrophysics today are
attempts to detect dark matter, and there seems to be a lot of it in the universe.
So there's some hope that physicists will make headway on its composition
within the foreseeable future.
Detecting cosmic superstrings
Cosmic strings (which in this case are not the same things as the fundamental
superstrings of string theory) were originally proposed in 1976 by Tom
Kibble of Imperial College London, who suggested that in the aftermath of the
big bang, as the universe went through a rapid cooling phase, defects may
have remained behind. These defects in quantum fields are similar to when
you rapidly freeze water into ice, creating a white substance that is full of
defects.
For a while in the 1980s, some scientists thought cosmic strings might be the
original seed material for galaxies, but the CMBR data doesn't indicate this
to be true. Years later, string theory would resurrect the notion of cosmic
strings in a new form.
According to some string theory models, superstrings created in the big bang
may have expanded along with the universe itself, creating cosmic superstrings.
An alternate explanation explains these cosmic superstrings as remnants
from the collision of two branes.
.Chapter 12: Putting String Theory to the Test ££,3
Cosmic superstrings would be incredibly dense objects. Narrower than a
proton, a single meter of a cosmic superstring could weigh about the same as
North America. As they vibrated in space, they could generate massive gravity
waves rippling out through space-time.
One way of seeing the cosmic superstrings would be through the gravitational
lensing, where the string's gravity bends the light of a star, as shown in
Figure 12-2. This might mean that we see one star in two different locations,
each equally bright.
According to Joe Polchinski, the best way to look for cosmic superstrings is
to observe pulsars (such as the ones that Fermi is detecting, as mentioned
earlier in this chapter). Pulsars are like astronomical lighthouses, spinning as
they fire regular beams of electromagnetic radiation into the universe, which
follow a predictable pattern. The gravity from a cosmic superstring could
cause ripples in space-time that alter this pattern in a way that should be
detectable here on Earth.
Looking for Evidence Closer to Home:
Using Particle Accelerators
Although it would be nice if nature gave us the experimental results we need,
scientists are never content to wait for a lucky break, which is why they
proceed with experiments in apparatuses that they control. For high-energy
particle physics, this means particle accelerators.
A particle accelerator is a device that uses powerful magnetic fields to
accelerate a beam of charged particles up to incredibly fast speeds and then
collides it with a beam of particles going the other way. Scientists can then
analyze the results of the collision.
22&# P art '" : Building String Theory: A Theory of Everything
Relativistic HeaVy Ion Collider (RHlC)
The Relativistic Heavy Ion Collider (RHIC) is a particle accelerator at
Brookhaven National Laboratory in New York. It went online in 2000, after a
decade of planning and construction.
The RHIC name comes from the fact that it accelerates heavy ions — that
is, atomic nuclei stripped of their electrons — at relativistic speeds (99.995
percent the speed of light) and then collides them. Because the particles are
atomic nuclei, the collisions contain a lot of power in comparison to pure
proton beams (though it also takes more time and energy to get them up to
that speed).
By slamming two gold nuclei together, physicists can obtain a temperature
300 million times hotter than the sun's surface. The protons and neutrons
that normally make up the nuclei of gold break down at this temperature into
a plasma of quark and gluons.
This quark-gluon plasma is predicted by quantum chromodynamics (QCD),
but the problem is that the plasma is supposed to behave like a gas. Instead,
it behaves like a liquid. According to Leonard Susskind, string theory
may be able to explain this behavior using a variation on the Maldacena
conjecture (described in Chapter 11). In this way, the quark-gluon plasma
may be described by an equivalent theory in the higher-dimensional universe:
a black hole, in this case!
These results are far from conclusive, but theorists are looking at the
behavior of these collisions to find ways to apply string theory to make
greater sense of the existing physical models (QCD in this case), which is a
powerful tool to help gain support of string theory.
Large Hadron Collider (LHC)
The Large Hadron Collider (LHC) is a massive apparatus, built underground
at the CERN particle physics facility on the border of Switzerland and France.
(CERN is the European particle physics center that was, in 1968, the birthplace
of string theory.) The accelerator itself is about 27 kilometers (17 miles) in
circumference, as shown in Figure 12-3. The 9,300 magnets of the facility can
accelerate protons into collisions up to possibly 14 trillion electron volts
(TeV), well beyond our current experimental limitations. The cost of the LHC
was around $9 billion as of this writing.
.Chapter 12: Putting String Theory to the Test 225
On September 10, 2008, the LHC came online by officially running a beam
the full length of the tunnel. On September 19, a faulty electrical connection
caused a rupture in the vacuum seal, resulting in a leak of 6 tons of liquid
helium. The repairs (and upgrades to avoid the problem in the future) were
scheduled to take at least a year.
Due to this, there have yet to be any significant experimental results from the
LHC, but they should be coming in the next year or so. The 14 TeV energy
level might be able to reach several possible experimental results:
j-" Microscopic black holes, which would support predictions of extra
dimensions
i"* Supersymmetric particle (sparticle) creation
U* Experimental confirmation of the Higgs boson, the final Standard Model
particle to remain unobserved
v* Evidence of curled-up extra dimensions
One of the greatest pieces of evidence for string theory could actually be
a lack of evidence. If the experiments at the LHC register some "missing
energy," a couple of possibilities could provide amazing support for string
theory.
226
Part III: Building String Theory: A Theory of Everything _
11^ First, the collisions could create new sparticles that form dark matter,
which then flows out of the facility without interacting with the normal
matter (like, you know, the detector itself).
J-" Second, missing energy could result from energy (or sparticles) that are
actually traveling directly into the extra dimensions, rather than into our
own 4-dimensional space-time.
Either of these findings would be a great discovery, and either the
supersymmetric particles or extra dimensions would have profound
implications for string theory.
Colliders of the future
Particle accelerators are so massive that there are no set designs for them;
each particle accelerator is its own prototype. The next one on the books
appears to be the International Linear Collider (ILC), which is an electron-
positron collider. One benefit of this is that electrons and positrons, because
they're fundamental particles and not composite particles like protons, are a
lot less messy when they collide.
The ILC has not been approved. Proposals, including location, could be voted
on around 2012 and, if approved, it could be running in the late 2010s. Early
estimates for the project give a minimum cost of $6.65 billion (excluding little
things like actually buying the land and other incidental costs).
It's also possible that the LHC might be the last of the large particle
accelerators, because new proposed technologies may be developed that
allow for rapid particle acceleration that doesn't require massive facilities.
One such design, proposed at CERN, is the Compact Linear Collider (CLIC).
The CLIC would use a new two-beam accelerator, where one beam accelerates
a second beam. The energy from a low-energy (but high-current) beam into
a high-energy (but low-current) beam could allow for accelerations up to
5 TeV in a much shorter distance than traditional accelerators. A decision on
CLIC could be made in 2010, with construction probably completed shortly
after 2020.
Part IV
The Unseen Cosmos: String
Theory On the Boundaries
of Knowledge
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In this part .
String theory brings up many amazing possibilities
about how to explain the fundamental properties of
our universe, such as space, time, and matter itself.
Though physicists are far from reaching a final version of
string theory, there are many possible implications worth
thinking about, even at this early stage in the theory's
development.
In this part, I explore the implications of string theory on
our view of the universe. I explain how mathematicians
and scientists use the concept of dimensions and how the
extra dimensions in string theory can be interpreted.
Then I return to the ideas of cosmology and show how
string theory presents possible explanations for properties
in our universe.
String theory can also be used as a means of presenting
the ideas of other universes, some of which may in theory
someday be accessible. Finally, I discuss the possibility of
whether string theory could ever allow for time travel.
Chapter 13
Making Space for
Extra Dimensions
In This Chapter
Understanding the meaning of dimensions
Adding a time dimension to the space dimensions
Bending dimensions as a mathematic pastime
Offering alternatives to extra dimensions
■ Mne of the most fascinating aspects of string theory is the requirement of
^^ extra dimensions to make the theory work. String theory requires nine
space dimensions, while M-theory seems to require ten space dimensions.
Under some theories, some of these extra dimensions may actually be long
enough to interact with our own universe in a way that could be observed.
In this chapter, you get a chance to explore and understand the meaning of
these extra dimensions. First, I introduce the concept of dimensions in a very
general way, talking about different approaches mathematicians have used to
study 2- and 3-dimensional space. Then I tackle the idea of time as the fourth
dimension. I analyze the ways in which the extra dimensions may manifest in
string theory and whether the extra dimensions are really necessary.
What Are dimensions)
Any point in a mathematical space can be defined by a set of coordinates,
and the number of coordinates required to define that point is the number of
dimensions the space possesses. In a 3-dimensional space like you're used to,
for example, every point can be uniquely defined by precisely three coordi-
nates — three pieces of information (length, width, and height). Each dimen-
sion represents a degree of freedom within the space.
Though I've been talking about dimensions in terms of space (and time),
the concept of dimensions extends far beyond that. For example, the match-
making Web site eHarmony.com provides a personality profile that claims to
^3 P art '^ : The Unseen Cosmos: String Theory On the Boundaries of Knowledge
assess you on 29 dimensions of personality. In other words, it uses 29 pieces
of information as parameters for its dating matches.
I don't know the details of eHarmony's system, but I have some experience
with using dimensions on other dating sites. Say you wanted to find a potential
romantic partner. You're trying to target a specific type of person by entering
different pieces of information: gender, age range, location, annual income,
education level, number of kids, and so on. Each of these pieces of informa-
tion narrows down the "space" that you're searching on the dating site. If you
have a complete space consisting of every single person who has a profile on
the dating site, when your search is over you're narrowed to searching only
among those who are within the ranges that you've specified.
Say Jennifer is a female, age 30, in Dallas, with a college degree and one child.
Those coordinates "define" Jennifer (at least to the dating site), and searches
that sample those coordinates will include Jennifer as one of the "points" (if
you think of each person as a point) in that section of the space.
The problem with this analogy is that you end up with a large number of
points within the dating site space that have the same coordinates. There
may be another girl, Andrea, who enters essentially identical information as
Jennifer. Any search of the sample space that brings up Jennifer also brings
up Andrea. In the physical space that we live in, each point is unique.
^jjUBEfl Each dimension — in both mathematics and in the dating site example — rep-
resents a degree of freedom within the space. By changing one of the coordi-
nates, you move through the space along one of the dimensions. For example,
you can exercise a degree of freedom to search for someone with a different
educational background or a different age range or both.
When scientists talk about the number of dimensions in string theory, they
mean the degrees of freedom required for these theories to work without
going haywire. In Chapter 10, 1 explain that the bosonic string theory required
25 space dimensions to be consistent. Later, superstring theory required 9
space dimensions. M-theory seems to require 10 space dimensions, and the
later F-theory includes 12 total dimensions.
2-bimensional Space: Exploring
the Geometry of Ftattand
Many people think of geometry (the study of objects in space) as a flat,
2-dimensional space that contains two degrees of freedom — up or down and
right or left. Throughout most of modern history, this interest has been the
study of Euclidean geometry or Cartesian geometry.
_Chapter 13: Making Space for Extra Dimensions ^3 *
Euclidean geometry: Think back
to high school geometry
Probably the most famous mathematician of the ancient world was Euclid,
who has been called the father of geometry. Euclid's 13-volume book,
Elements, is the earliest known book to have taken all the existing knowledge
of geometry at the time of its writing (around 300 BCE). For nearly 2,000
years, virtually all of geometry could be understood just by reading Elements,
which is one reason why it was the most successful math book ever.
In Elements, Euclid started off presenting the principles of plane geometry —
that is, the geometry of shapes on a flat surface, as in Figure 13-1. An impor-
tant consequence of Euclidean plane geometry is that if you take the measure
of all three angles inside of a triangle, they add up to 180 degrees.
Later in the volumes, Euclid extended into 3-dimensional geometry of solid
objects, such as cubes, cylinders, and cones. The geometry of Euclid is the
geometry typically taught in school to this day.
Cartesian geometry: Merging algebra
and Euclidean geometry
Modern analytic geometry was founded by French mathematician and phi-
losopher Rene Descartes, when he placed algebraic figures on a physical
grid. This sort of Cartesian grid is shown in Figure 13-2. By applying concepts
from Euclidean geometry to the equations depicted on the grids, insights into
geometry and algebra could be obtained.
^3 <s- P art 'V: The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
Around the same time that Galileo was revolutionizing the heavens,
Descartes was revolutionizing mathematics. Until his work, the fields of alge-
bra and geometry were separate. His idea was to display algebraic equations
graphically, providing a way to translate between geometry and algebra.
Books of many dimensions
The book Flatland: A Romance of Many
Dimensions by Edwin A. Abbott, written in 1884,
is a classic in the mathematics community for
explaining the concept of multiple dimensions.
In this book, A. Square lives in a flat world
and gains perspective when he encounters a
sphere passing through his world who pulls
him out of it so he can briefly experience three
dimensions.
Flatland appears to have been part of a grow-
ing popular culture interest in extra dimensions
during the late 1800s. Lewis Carroll had written
a story in 1865 entitled "Dynamics of a Particle,"
which included 1-dimensional beings on a flat
surface, and the idea of space going crazy is
clearly a theme in Carroll's Alice's Adventures
in Wonderland (1865) and Through the Looking
Glass (1872). Later, H. G. Wells used the con-
cepts of extra dimensions in several stories,
most notably in The Time Machine (1895),
where time is explicitly described as the fourth
dimension a full decade before Einstein pre-
sented the first inkling of relativity.
Various independent sequels have been writ-
ten to Flatland through the years to expand on
the concept. These include Dionys Burger's
Sphereland (1965), Ian Stewart's Flatterland
(2001), and Rudy Rucker's Spaceland (2002). A
related book is the 1984 science-fiction novel
The Planiverse, where scientists in our world
establish communication with a Flatland-like
world.
_Chapter 13: Making Space for Extra Dimensions ^ J J
Using the Cartesian grid, you can define a line by an equation; the line is the
set of solutions to the equation. In Figure 13-2, the line goes from the origin
to the point (5, 3). Both the origin (0, 0) and (5, 3) are correct solutions to the
equation depicted by the line (along with all the other points on the line).
Because the grid is 2-dimensional, the space that the grid represents contains
two degrees of freedom. In algebra, the degrees of freedom are represented
by variables, meaning that an equation that can be shown on a 2-dimensional
surface has two variable quantities, often x and y.
Three Dimensions of Space
When looking in our world, it has three dimensions — up and down, left and
right, back and forth. If you give a longitude, latitude, and an altitude, you can
determine any location on Earth, for example.
A straight line in space: Vectors
Expanding on the idea of Cartesian geometry, you find that it's possible
to create a Cartesian grid in three dimensions as well as two, as shown in
Figure 13-3. In such a grid, you can define an object called a vector, which has
both a direction and a length. In 3-dimensional space, every vector is defined
by three quantities.
Figure 13-3:
It takes
three
numbers
to define a
vector (or
location)
in three
dimensions.
2jli Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
Vectors can, of course, exist in one, two, or more than three dimensions.
(Technically, you can even have a zero-dimensional vector, although it will
always have zero length and no direction. Mathematicians call such a case
"trivial.")
Treating space as containing a series of straight lines is probably one of the
most basic operations that can take place within a space. One early field of
mathematics that focuses on the study of vectors is called linear algebra,
which allows you to analyze vectors and things called vector spaces of any
dimensionality. (More advanced mathematics can cover vectors in more
detail and extend into nonlinear situations.)
One of the major steps of working with vector spaces is to find the basis for
the vector space, a way of defining how many vectors you need to define any
point in the entire vector space. For example, a 5-dimensional space has a
basis of five vectors. One way to look at superstring theory is to realize that
the directions a string can move can only be described with a basis of ten dis-
tinct vectors, so the theory describes a 10-dimensional vector space.
Twisting 2-dimensionat space in three
dimensions: The Mobius strip
In the classic book Flatland, the main character is a square (literally — he
has four sides of equal length) who gains the ability to experience three
dimensions. Having access to three dimensions, you can perform actions on
a 2-dimensional surface in ways that seem very counterintuitive. A 2-dimen-
sional surface can actually be twisted in such a way that it has no beginning
and no end!
The best known case of this is the Mobius strip, shown in Figure 13-4. The
Mobius strip was created in 1858 by German mathematicians August
Ferdinand Mobius and Johann Benedict Listing.
_Chapter 13: Making Space for Extra Dimensions 2j3
You can create your own Mobius strip by taking a strip of paper — kind of like
a long bookmark — and giving it a half-twist. Then take the two ends of the
strip of paper and tape them together. Place a pencil in the middle of the sur-
face and draw a line along the length of the strip without taking your pencil off
the paper.
A curious thing happens as you continue along. Eventually, without taking
your pencil from the paper, the line is drawn on every part of the surface and
eventually meets up with itself. There is no "back" of the Mobius strip, which
somehow avoids the pencil line. You've drawn a line along the entire shape
without lifting your pencil.
In mathematical terms (and real ones, given the result of the pencil experi-
ment), the Mobius strip has only one surface. There is no "inside" and "out-
side" of the Mobius strip, the way there is on a bracelet. Even though the two
shapes may look alike, they are mathematically very different entities.
The Mobius strip does, of course, have an end (or boundary) in terms of
its width. In 1882, the German mathematician Felix Klein expanded on the
Mobius strip idea to create a Klein bottle: a shape that has no inside or out-
side surface, but also has no boundaries in any direction. Take a look at
Figure 13-5 to understand the Klein bottle. If you traveled along the "front" of
the path (with the x's), you'd eventually reach the "back" of that path (with
the o's).
If you were an ant living on a Mobius strip, you could walk its length and even-
tually get back to where you started. Walking its width, you'd eventually run
into the "edge of the world." An ant living on a Klein bottle, however, could go
in any direction and, if it walked long enough, eventually find itself back where
it started. (Traveling along the o path eventually leads back to the x's.) The
2j0 P art '^ : The Unseen Cosmos: String Theory On the Boundaries of Knowledge
difference between walking on a Klein bottle and walking on a sphere is that
the ant wouldn't just walk along the outside of the Klein bottle, like it would on
a sphere, but it would cover both surfaces, just like on the Mobius strip.
More twists in three dimensions:
Non-Euctidean geometry
The fascination with strange warping of space in the 1800s was perhaps
nowhere as clear as in the creation of non-Euclidean geometry, where math-
ematicians began to explore new types of geometry that weren't based on
the rules laid out 2,000 years earlier by Euclid. One version of non-Euclidean
geometry is Riemannian geometry, but there are others, such as projective
geometry.
The reason for the creation of non-Euclidean geometry is based in Euclid's
Elements itself, in his "fifth postulate," which was much more complex than the
first four postulates. The fifth postulate is sometimes called the parallel postu-
late and, though it's worded fairly technically, one consequence is important
for string theory's purposes: A pair of parallel lines never intersects.
Well, that's all well and good on a flat surface, but on a sphere, for example,
two parallel lines can and do intersect. Lines of longitude — which are
parallel to each other under Euclid's definition — intersect at both the
north and south poles. Lines of latitude, also parallel, don't intersect at all.
Mathematicians weren't sure what a "straight line" on a circle even meant!
One of the greatest mathematicians of the 1800s was Carl Friedrich Gauss,
who turned his attention to ideas about non-Euclidean geometry. (Some ear-
lier thoughts on the matter had been kicked around over the years, such as
those by Nikolai Lobachevsky and Janos Bolyai.) Gauss passed the majority
of the work off to his former student, Bernhard Riemann. Riemann worked
out how to perform geometry on a curved surface — a field of mathematics
called Riemannian geometry. One consequence — that the angles of a triangle
do not add up to 180 degrees — is depicted in Figure 13-6.
the angles
of a triangle
sure up to
180 degrees.
o
_Chapter 13: Making Space for Extra Dimensions ^3 I
The mathematics of artwork
Understanding and manipulating space is a
key feature of artwork, which often attempts
to reflect a 3-dimensional reality on a 2-dimen-
sional surface. This is probably most notable
in the work of Pablo Picasso and M. C. Escher,
where space has been manipulated in such a
way that the manipulation itself is part of the
artistic message.
Most artists try to manipulate space so it's not
noticed. One of the most common examples
of this is perspective, developed during the
Renaissance, which involves creating an image
that matches the way the eye perceives space
and distance. Parallel railroad tracks appearto
meet at the horizon, though they never meet in
reality. On a 2-dimensional surface, the basis
for the railroad tracks is a triangle that does, in
fact, have a corner at the horizon line.
This is precisely the basis of the mathemati-
cal field of non-Euclidean geometry called
projective geometry, where you take one
2-dimensional space and project it in a pre-
cise mathematical way onto a second sur-
face. There is an exact 1 -to - 1 correspondence
between the two spaces, even though they look
completely different. The two images represent
different mathematical ways of looking at the
same physical space — one of them an infinite
space and one a finite space.
When Albert Einstein developed general relativity as a theory about the
geometry of space-time, it turned out that Riemannian geometry was exactly
what he needed.
Four dimensions of Space-Time
In Einstein's general theory of relativity, the three space dimensions connect
to a fourth dimension: time. The total package of four dimensions is called
space-time, and in this framework, gravity is seen as a manifestation of space-
time geometry. The story of relativity is told in Chapter 6, but some dimen-
sion-related points are worth revisiting.
Hermann Minkowski, not Albert Einstein, realized that relativity could be
expressed in a 4-dimensional space-time framework. Minkowski was one of
Einstein's old teachers, who had called him a "lazy dog," but he clearly saw
the brilliance of relativity.
In a 1908 talk entitled "Space and Time," Minkowski first broached the topic
of creating a dimensional framework of space-time (also sometimes called a
"Minkowski space"). The Minkowski diagrams, introduced in Chapter 6, are
an attempt to graphically represent this 4-dimensional space on a 2-dimen-
sional Cartesian grid. Each point on the grid is a "space-time event," and
2jO P art IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
understanding the ways these events relate to each other is the goal of ana-
lyzing relativity in this way.
Even though time is a dimension, it's fundamentally different from the space
dimensions. Mathematically, you can generally exchange "left" for "up" and
end up with results that are fairly consistent. If you, however, exchange "left
one meter" for "one hour from now," it doesn't work out so well. Minkowski
divided the dimensions into spacelike dimensions and timelike dimen-
sions. One spacelike dimension can be exchanged for another, but can't be
exchanged with a timelike dimension. (In Chapter 16, you find out about some
ideas regarding extra timelike dimensions in our universe.)
The reason for this distinction is that Einstein's equations are written in such
a way that they result in a term defined by the space dimensions squared
minus a term defined by the time dimension squared. (Because the terms are
squared, each term has to be positive, no matter what the value of the dimen-
sion.) The space dimensional values can be exchanged without any math-
ematical problem, but the minus sign means that the time dimension can't be
exchanged with the space dimensions.
Adding More dimensions
to Make a Theory Work
For most interpretations, superstring theory requires a large number of
extra space dimensions to be mathematically consistent: M-theory requires
ten space dimensions. With the introduction of branes as multidimensional
objects in string theory, it becomes possible to construct and imagine wildly
creative geometries for space — geometries that correspond to different pos-
sible particles and forces. It's unclear, at present, whether those extra dimen-
sions exist in a real sense or are just mathematical artifacts.
^jftBEfl The reason string theory requires extra dimensions is that trying to elimi-
' y ^X nate them results in much more complicated mathematical equations. It's
jjljj ) not impossible (as you see later in this chapter), but most physicists haven't
pursued these concepts in a great deal of depth, leaving science (perhaps by
default) with a theory that requires many extra dimensions.
As I mention earlier, from the time of Descartes, mathematicians have
been able to translate between geometric and physical representations.
Mathematicians can tackle their equations in virtually any number of dimen-
sions that they choose, even if they can't visually picture what they're talking
about.
_Chapter 13: Making Space for Extra Dimensions 23 •
One of the tools mathematicians use in exploring higher dimensions is anal-
ogy. If you start with a zero-dimensional point and extend it through space,
you get a 1-dimensional line. If you take that line and extend it into a second
dimension, you end up with a square. If you extend a square through a third
dimension, you end up with a cube. If you then were to take a cube and extend
into a fourth dimension, you'd get a shape called a hypercube.
A line has two "corners" but extending it to a square gives four corners, while
a cube has eight corners. By continuing to extend this algebraic relationship,
a hypercube would be a 4-dimensional object with 16 corners, and a similar
relationship can be used to create analogous objects in additional dimen-
sions. Such objects are obviously well outside of what our minds can picture.
Humans aren't psychologically wired to be able to picture more than three
space dimensions. A handful of mathematicians (and possibly some physi-
cists) have devoted their lives to the study of extra dimensions so fully that
they may be able to actually picture a 4-dimensional object, such as a hyper-
cube. Most mathematicians can't (so don't feel bad if you can't).
Whole fields of mathematics — linear algebra, abstract algebra, topology,
knot theory, complex analysis, and others — exist with the sole purpose of
trying to take abstract concepts, frequently with large numbers of possible
variables, degrees of freedom, or dimensions, and make sense of them.
These sorts of mathematical tools are at the heart of string theory.
Regardless of the ultimate success or failure of string theory as a physical
model of reality, it has motivated mathematics to grow and explore new
questions in new ways, and for that alone, it has proved useful.
Sending Space and lime on a Bender
Space-time is viewed as a smooth "fabric," but that smooth fabric can be
bent and manipulated in various ways. In relativity, gravity bends our four
space-time dimensions, but in string theory more dimensions are bound up
in other ways. In relativity and modern cosmology, the universe has an inher-
ent curvature.
The typical approach to string theory's extra dimensions has been to wind
them up in a tiny, Planck length-sized shape. This process is called compac-
tification. In the 1980s, it was shown that the extra six space dimensions of
superstring theory could be compactified into Calabi-Yau spaces.
^ySTo A Since then, other methods of compactification have been offered, most nota-
bly G2 compactification, spin-bundle compactification, and flux compactifica-
tion. For the purposes of this book, the details of the compactification don't
matter.
4m tX P art 'V: The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
The wraparound universe
Some cosmologists have considered some
extreme cases of space warping in our own
universe, theorizing that the universe may be
smaller than we think. A new field of cosmol-
ogy called cosmic topology attempts to use
mathematical tools to study the overall shape
of the universe.
In his 2008 book, The Wraparound Universe,
cosmologist Jean-Pierre Luminet proposes the
idea that our universe wraps around so it has no
particular boundary, sort of like the Klein bottle
in Figure 13-5. Any direction you look, you may
be seeing an illusion, as if you were standing in
a funhouse full of mirrors that appeared to go
on forever. Distant stars may actually be closer
than expected, but the lighttravels a larger path
along the wraparound universe to reach us.
In this sort of a scenario, the horizon problem
from Chapter 9 ceases to be an issue because
the universe is small enough to have become
uniform within the timeframe of our universe's
existence. Inflation is consistent with the wrap-
around universe hypothesis, but many of the
problems it fixes are solved in other ways.
To picture compactification, think of a garden hose. If you were an ant living
on the hose, you'd live on an enormous (but finite) universe. You can walk
very far in either of the length directions, but if you go around the curved
dimension, you can only go so far. However, to someone very far away, your
dimension — which is perfectly expansive at your scale — seems like a very
narrow line with no space to move except along the length.
This is the principle of compactification — we can't see the extra universes
because they're so small that nothing we can do can ever distinguish them as
a complex structure. If we got close enough to the garden hose, we'd realize
that something was there, but scientists can't get close to the Planck length
to explore extra compactified dimensions.
Of course, some recent theories have proposed that the extra dimensions may
be larger than the Planck length and theoretically in the range of experiment.
Still other theories exist in which our region of the universe only manifests
four dimensions, even though the universe as a whole contains more. Other
regions of the universe may exhibit additional dimensions. Some radical theo-
ries even suppose that the universe as a whole is curved in strange ways.
Are Extra Dimensions Realty Necessary}
Though string theory implies extra dimensions, that doesn't mean that the
extra dimensions need to exist as dimensions of space. Some work has been
done to formulate a 4-dimensional string theory where the extra degrees of
_Chapter 13: Making Space for Extra Dimensions <£[l /
freedom aren't physical space dimensions; but the results are incredibly
complex, and it doesn't seem to have caught on.
Several groups have performed this sort of work, because some physicists
are uncomfortable with the extra space dimensions that seem to be required
by string theory. In the late 1980s, a group worked on an approach called free
fermions. Other approaches that avoid introducing additional dimensions
include the covariant lattice technique, asymmetric orbifolds, the 4-D 7V=2
string (what's in a name?), and non-geometric compactifications. These are
technically complex formulations of string theory (aren't they all?) that seem
to be ignored by virtually all popular books on the subject, which focus on
the idea of extra dimensions to the exclusion of these alternative approaches.
Even among string theorists, the geometric approach of compactifying extra
dimensions is the dominant approach.
One early, technically complex (and largely ignored) approach to 4-dimen-
sional string theory is work performed by S. James Gates Jr., of the University
of Maryland at College Park (along with assistance from Warren Siegel of
Stony Brook University's C. N. Yang Institute for Theoretical Physics). This
work is by no means the dominant approach to 4-dimensional string theory,
but it's benefit is that it can be explained and understood (in highly simpli-
fied terms) without a doctorate in theoretical physics.
Offering an alternative
to multiple dimensions
In Gates's approach, he essentially trades dimensions for charges. This cre-
ates a sort of dual approach that's mathematically similar to the approach in
extra space dimensions, but doesn't actually require the extra space dimen-
sions nor require guessing at compactification techniques to eliminate the
extra dimensions.
This idea dates back to a 1938 proposal by British physicist Nicolas Kemmer.
Kemmer proposed that the quantum mechanical properties of charge and
spin were different manifestations of the same thing. Specifically, he said that
the neutron and proton were identical, except that they rotated differently
in some extra dimension, which resulted in a charge on the proton and no
charge on the neutron. The resulting mathematics, which analyzes the physi-
cal properties of these particles, is called an isotopic charge space (originally
developed by Werner Heisenberg and Wolfgang Pauli, then used by Kemmer).
Though this is an "imaginary space" (meaning that the coordinates are unob-
servable in the usual sense), the resulting mathematics describes properties
of protons and neutrons, and is at the foundation of the current Standard
Model.
Jill £ Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
Gates's approach was to take Kemmer's idea in the opposite direction: If you
wanted to get rid of extra dimensions, perhaps you could view them as imagi-
nary and get charges. (The word "charge" in this sense doesn't really mean
electrical charge, but a new property to be tracked, like "color charge" in
QCD.) The result is to take vibrational dimensions of the heterotic string and
view them as "left charge" and "right charge."
When Gates applied this concept to the heterotic string, the trading didn't
come out even — to give up six space dimensions, he ended up gaining more
than 496 right charges!
In fact, together with Siegel, Gates was able to find a version of heterotic
string theory that matched these 496 right charges. Furthermore, their solu-
tion showed that the left charges would correspond to the family number.
(There are three known generations, or families, of leptons as shown in
Figure 8-1 in Chapter 8 — the electron, muon, and tau families. The family
number indicates which generation the particle belongs to.)
This may explain why there are multiple families of particles in the Standard
Model of particle physics. Based on these results, a string theory in four
dimensions could require extra particle families! In fact, it would require many
more particle families than the three that physicists have seen. These extra
families (if they exist) could include particles that could make up the unseen
dark matter in our universe.
Weighing fewer dimensions
against simpler equations
The usefulness of these 4-dimensional results is hindered by the sheer com-
plexity of the resulting equations (even by string theory standards). Although
all string theories are complex, 4-dimensional string theories have, to date,
shown meager predictive power. Assuming the extra dimensions lead to
equations that are easier to handle, most physicists choose to work under
the assumption of greater numbers of dimensions.
This goes back to the idea that the principle of Occam's razor, which says
that a scientist shouldn't make a theory unnecessarily complex. The simplest
explanation that fits the facts is the one that physicists tend to gravitate
toward.
In this case, Occam's razor cuts both ways. The simpler mathematical equa-
tion of 10-dimensional string theory requires stipulating a large number of
space dimensions that no one has ever observed, which would certainly
_Chapter 13: Making Space for Extra Dimensions 2£ij
seem to go against Occam's razor. But the type of isotopic charge coordi-
nate used in Gates's approach is exactly the same as the ones that provide
the mathematical foundations of the Standard Model — where the isotopic
dimensions aren't observed.
In the end, the 4-dimensional interpretations of string theory are a powerful
way of understanding how complex string theory can be. One of the most
basic aspects of string theory has been the idea that it requires extra space
dimensions, but this work shows that string theory doesn't necessarily
require even that. If these approaches are right, and the degrees of freedom
inherent in the theory don't require extra space dimensions, then the physi-
cal principles at the heart of string theory may be completely unexpected.
4m ti ti P art IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
Chapter 14
Our Universe — String Theory,
Cosmology, and Astrophysics
In This Chapter
Looking back beyond the big bang theory
Tying black holes to string theory
Knowing where the universe has been and where it may be going
Tackling the question of how the universe supports life
Though string theory started as a theory of particle physics, much of the
significant theoretical work today is in applying the startling predictions
of string theory and M-theory to the field of cosmology. Chapter 9 covered
some of the amazing facts science has discovered about our universe, espe-
cially in the last century.
In this chapter, I return to these same ideas from the background of string
theory. I explain how string theory relates to our understanding of the big
bang, the theory of the universe's origin. I then discuss what string theory
has to say about another mystery of the universe — black holes. From there,
I cover what string theory reveals about how the universe changes over time
and how it may change in the future. Finally, I return to the question of why
the universe seems perfectly tuned to allow for life and what, if anything,
string theory (along with the anthropic principle) may have to say about it.
The Start of the Universe
u/ith String Theory
According to the big bang theory, if you extrapolate the expanding universe
backward in time, the entire known universe would have been compacted
down into a singular point of incredibly immense density. It reveals nothing,
however, about whether anything existed a moment prior to that point.
In fact, under the big bang theory — formulated in a universe of quantum
2/4 V ' >art '^ : The Unseen Cosmos: String Theory On the Boundaries of Knowledge
physics and relativity — the laws of physics result in meaningless infinities at
that moment. String theory may offer some answers to what came before and
what caused the big bang.
What Was before the banq}
String theory offers the possibility that we are "stuck" on a brane with three
space dimensions. These brane world scenarios, such as the Randall-Sundrum
models, offer the possibility that before the big bang something was already
here: collections of strings and branes.
The search for an eternal universe
Scientists were originally very upset by the big bang theory, because they
believed in an eternal universe, meaning that the universe had no starting
point (and, on average, didn't change over time). Einstein believed this,
though he abandoned it when evidence suggested otherwise. Fred Hoyle
devoted most of his career to trying to prove the universe was eternal.
Today, some physicists continue to look for ways to explain what, if anything,
existed before the big bang.
Some cosmologists say that the question of what happened at or before the
big bang is inherently unscientific, because science currently has no way of
extending its physical theories past the singularity at the dawn of our uni-
verse's timeline. Others point out that if we never ask the questions, we'll
never discover a way to answer them.
Though string theory isn't yet ready to answer such questions, that hasn't
stopped cosmologists from beginning to ask the questions and offer possible
scenarios. In these scenarios, which are admittedly vague, the pre-big bang
universe (which likely is not confined to only three space dimensions) is a
conglomerate of p-branes, strings, anti-strings, and anti-p-branes. In many
cases, these objects are still "out there" somewhere beyond our own 3-brane,
perhaps even impacting our own universe (as in the case of the Randall-
Sundrum models).
One of these models was a pre-big bang model presented by Gabriele
Veneziano — the same physicist who came up with the 1968 dual resonance
model that sparked string theory. In this model, our universe is a black hole
in a more massive universe of strings and empty space. Prior to the current
expansion phase, there was a period of contraction. Though probably not
completely true according to today's major models, this work by Veneziano
(and similar ideas by others) has an impact on most of the superstring cos-
mology work today, because it pictures our known universe as just a subset
of the universe, with a vast "out there" beyond our knowledge.
.Chapter 14: Our Universe — String Theory, Cosmology, and Astrophysics £U. /
The old-fashioned cyclic universe model
One idea that was popular in the 1930s was that of a cyclic universe, in which
the matter density was high enough for gravity to overcome the expansion of
the universe. The benefit of this model was that it allowed the big bang to be
correct, but the universe could still be eternal.
In this cyclic model, the universe would expand until gravity began to pull it
back, resulting in a "big crunch" where all matter returned to the primordial
"superatom" — and then the cycle of expansion would start all over again.
The problem is that the second law of thermodynamics dictates that the
entropy, or disorder, in the universe would grow with each cycle. If the
universe went through an infinite number of cycles, the amount of disorder
in the universe would be infinite — every bit of the universe would be in
thermal equilibrium with every other bit of the universe. In a universe where
every region has exactly the same structure, no one region has more order
than any other, so all regions have the maximum amount of disorder allowed.
(If the universe had gone through a finite number of cycles, scientists still
ran into the problem of how the whole thing started; they just pushed it back
a few cycles. This kind of defeated the whole purpose of the model, so the
model assumed an infinite number of cycles.)
String theory, however, might just have a way of bringing back the cyclic
model in a new form.
What banged}
The big bang theory doesn't offer any explanation for what started the origi-
nal expansion of the universe. This is a major theoretical question for cos-
mologists, and many are applying the concepts of string theory in attempts
to answer it. One controversial conjecture is a cyclic universe model called
the ekpyrotic universe theory, which suggests that our own universe is the
result of branes colliding with each other.
The banging of strings
Well before the introduction of M-theory or brane world scenarios, there
was a string theory conjecture of why the universe had the number of dimen-
sions we see: A compact space of nine symmetrical space dimensions began
expanding in three of those dimensions. Under this analysis, a universe with
three space dimensions (like ours) is the most likely space-time geometry.
In this idea, initially posed in the 1980s by Robert Brandenberger and
Cumrun Vafa, the universe began as a tightly wound string with all dimen-
sions symmetrically confined to the Planck length. The strings, in effect,
bound the dimensions up to that size.
Jill O Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
Brandenberger and Vafa argued that in three or fewer dimensions, it would
be likely for the strings to collide with anti-strings. (An anti-string is essen-
tially a string that winds in a direction opposite the string.) The collision
annihilates the string which, in turn, unleashes the dimensions it was confin-
ing. They thus begin expanding, as in the inflationary and big bang theories.
Instead of thinking about strings and anti-strings, picture a room that has
a bunch of cables attached to random points on the walls. Imagine that the
room wants to expand with the walls and floor and ceiling trying to move
away from each other — but they can't because of the cables. Now imagine
that the cables can move, and every time they intersect, they can recombine.
Picture two taut cables stretching from the floor to the ceiling that intersect to
form a tall, skinny X. They can recombine to become two loose cables — one
attached to the floor and one attached to the ceiling. If these had been the
only two cables stretching from floor to ceiling, then after this interaction, the
floor and ceiling are free to move apart from each other.
In the Brandenberger and Vafa scenario, this dimension (up-down), as well as
two others, are free to grow large. The final step is that in four or more space
dimensions, the moving strings will typically never meet. (Think about how
points moving in two space dimensions will probably never meet, and the
rationale gets extended to higher dimensions.) So this mechanism only works
to free three space dimensions from their cables.
In other words, the very geometry of string theory implies that this scenario
would lead to us seeing fewer than four space dimensions — dimensions
of four or more are less likely to go through the string/anti-string collisions
required to "liberate" them from the tightly bound configuration. The higher
dimensions continue to be bound up by the strings at the Planck length and
are therefore unseen.
With the inclusion of branes, this picture gets more elaborate and harder to
interpret. Research into this approach in recent years hasn't been reassuring.
Many problems arise when scientists try to embed this idea more rigorously
into the mathematics of string theory. Still, this is one of the few explanations
of why there are four dimensions that make any sense, so string theorists
haven't completely abandoned it as a possible reason for the big bang.
A brane-fueted, 2 ht-centuru cyclic model: The ekpyrotic universe
In the ekpyrotic universe scenario, our universe is created from the collision
of branes. The matter and radiation of our universe comes from the kinetic
energy created by the collision of these two branes.
The ekpyrotic universe scenario was proposed in a 2001 paper by
Paul Steinhardt of Princeton University, Burt Ovrut of the University of
Pennsylvania, and Neil Turok, formerly of Cambridge University and cur-
rently the director of the Perimeter Institute for Theoretical Physics in
Waterloo, Ontario, along with Steinhardt's student, Justin Khoury.
.Chapter 14: Our Universe — String Theory, Cosmology, and Astrophysics jtu. y
The theory builds on the ideas that some M-theory brane world scenarios
show that the extra dimensions of string theory may be extended, perhaps
even infinite in size. They are also probably not expanding (or at least string
theorists have no reason to think they are) the way that our own three space
dimensions are. When you play the video of the universe backward in time,
these dimensions don't contract.
Now imagine that within these dimensions you have two infinite 3-branes.
Some mechanism (such as gravity) draws the branes together through the
infinite extra dimensions, and they collide with each other. Energy is gener-
ated, creating the matter for our universe and pushing the two branes apart.
Eventually, the energy from the collision dissipates and the branes are drawn
back together to collide yet again.
The ekpyrotic model is divided into various epochs (periods of time), based
upon what influences dominate:
u* The big bang
U* The radiation-dominated epoch
j-" The matter-dominated epoch
V The dark energy-dominated epoch
J-" The contraction epoch
(-" The big crunch
The story up until the contraction epoch is essentially identical to that made
by regular big bang cosmology. The radiation that is spawned by the brane
collision (the big bang) means the radiation-dominated epoch is fairly uni-
form (save for quantum fluctuations), so inflation may be unnecessary. After
about 75,000 years, the universe becomes a particle soup during the matter-
dominated epoch. Today and for many years, we are in the dark energy-
dominated epoch, until the dark energy decays and the universe begins
contracting once again.
Because the theory involves two branes colliding, some called this the "big
splat" theory or the "brane smash" theory, which is certainly easier to pro-
nounce than ekpyrotic. The word "ekpyrotic" comes from the Greek word
"ekpyrosis," which was an ancient Greek belief that the world was born out of
fire. (Burt Ovrut reportedly thought it sounded like a skin disease.)
Some feel that the ekpyrotic universe model has a lot going for it — it solves
the flatness and horizon problems like inflationary theory does, while also
providing an explanation for why the universe started in the first place — but
the creators are still far from proving it. Stephen Hawking has bet Neil Turok
that findings from the European Space Agency's Planck satellite will verify
the inflationary model and rule out the ekpyrotic model, but Hawking has
been known to have to pay out on these sorts of bets in the past (as you can
230 P art 'V ; The Unseen Cosmos: String Theory On the Boundaries of Knowledge
read about in the "String theory and the black hole information paradox" sec-
tion later in this chapter).
One benefit is that this model avoids the problem of previous cyclic models,
because each universe in the cycle is larger than the one before it. Because
the volume of the universe increases, the total entropy of the universe in
each cycle can increase without ever reaching a state of maximum entropy.
There is obviously much more detail to the ekpyrotic model than I've included
here. If you're interested in this fascinating theory, I highly recommend Paul
J. Steinhardt and Neil Turok's popular book Endless Universe: Beyond the Big
Bang. In addition to the lucid and nontechnical discussion of complex scien-
tific concepts, their descriptions offer a glimpse inside the realm of theoretical
cosmology, which is well worth the read.
Explaining Black Hates
u/ith String Theory
One major mystery of theoretical physics that requires explanation is the
behavior of black holes, especially regarding how black holes evaporate and
whether they lose information. I introduce these topics in Chapter 9, but with
the concepts of string theory in hand, you may be able to further your under-
standing of them.
Black holes are defined by general relativity as smooth entities, but at very
small scales (such as when they evaporate down to the Planck length in size),
quantum effects need to be taken into account. Resolving this inconsistency
is the sort of thing that string theory should be good at, if it's true.
String theory and the thermodynamics
of a black hole
When Stephen Hawking described the Hawking radiation emitted by a black
hole, he had to use his physical and mathematical intuition, because quantum
physics and general relativity aren't reconciled. One of the major successes of
string theory is in offering a complete description of (some) black holes.
Hawking radiation takes place when radiation is emitted from a black hole,
causing it to lose mass. Eventually, the black hole evaporates into nothing (or
almost nothing).
.Chapter 14: Our Universe — String Theory, Cosmology, and Astrophysics 2 3 7
Stephen Hacking's incomplete argument
Hawking's paper on the way a black hole radiates heat (also called thermo-
dynamics) begins a line of reasoning that doesn't quite work all the way
through to the end. In the middle of the proof there's a disconnect, because
no theory of quantum gravity exists that would allow the first half of his rea-
soning (based on general relativity) to connect with the second half of his
reasoning (based on quantum mechanics).
The reason for the disconnect is that performing a detailed thermodynamics
analysis of a black hole involves examining all the possible quantum states
of the black hole. But black holes are described with general relativity, which
treats them as smooth — not quantum — objects. Without a theory of quan-
tum gravity, there seems to be no way to analyze the specific thermodynamic
nature of a black hole.
In Hawking's paper, this connection was made by means of his intuition, but
not in the sense that most of us probably think of intuition. The intuitive leap
he took was in proposing precise mathematical formulas, called greybody fac-
tors, even though he couldn't absolutely prove where they came from.
Most physicists agree that Hawking's interpretation makes sense, but a
theory of quantum gravity would show whether a more precise process
could take the place of his intuitive step.
String theory may complete the argument
Work by Andrew Strominger and Cumrun Vafa on the thermodynamics of
black holes is seen by many string theorists as the most powerful evidence in
support of string theory. By studying a problem that is mathematically equiv-
alent to black holes — a dual problem — they precisely calculated the black
hole's thermodynamic properties in a way that matched Hawking's analysis.
Sometimes, instead of simplifying a problem directly, you can create a dual
problem, which is essentially identical to the one you're trying to solve but is
much simpler to handle. Strominger and Vafa used this tactic in 1996 to calcu-
late the entropy in a black hole.
In their case, they found that the dual problem of a black hole described a col-
lection of 1-branes and 5-branes. These "brane constructions" are objects that
can be defined in terms of quantum mechanics. They found that the results
matched precisely with the result Hawking anticipated 20 years earlier.
Now, before you get too excited, the Strominger and Vafa results only work
for certain very specific types of black holes, called extremal black holes.
These extremal black holes have the maximum amount of electric or mag-
netic charge that is allowed without making the black hole unstable. An extre-
mal black hole has the odd property of possessing entropy but no heat or
temperature. (Entropy is a measure of disorder, often related to heat energy,
within a physical system.)
<£ J? <& P art IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
At the same time Strominger and Vafa were performing their calculations,
Princeton student Juan Maldacena was tackling the same problem (along
with thesis advisor Curt Callan). Within a few weeks of Strominger and Vafa,
they had confirmed the results and extended the analysis to black holes that
are almost extremal. Again, the relationship holds up quite well between
these brane constructions and black holes, and analyzing the brane construc-
tions yields the results Hawking anticipated for black holes. Further work has
expanded this work to even more generalized cases of black holes.
To get this analysis to work, gravity has to be turned down to zero, which cer-
tainly seems strange in the case of a black hole that is, quite literally, defined
by gravity. Turning off the gravity is needed to simplify the equations and
obtain the relationship. String theorists conjecture that by ramping up the
gravity again you'd end up with a black hole, but string theory skeptics point
out that without gravity you really don't have a black hole.
Still, even a skeptic can't help but think that there must be some sort of rela-
tionship between the brane constructions and the black holes because they
both follow the Hawking thermodynamics analysis created 20 years earlier.
What's even more amazing is that string theory wasn't designed to solve this
specific problem, yet it did. The fact that the result falls out of the analysis is
impressive, to say the least.
String theory and the black
hole information paradox
One of the important aspects of the thermodynamics of black holes relates to
the black hole information paradox. This paradox may well have a solution in
string theory, either in the string theory analyses described in the previous
section or in the holographic principle.
Hawking had said that if an object falls into a black hole, the only information
that is retained are the quantum mechanical properties of mass, spin, and
charge. All other information was stripped away.
The problem with this is that quantum mechanics is built on the idea that
information can't be lost. If information can be lost, then quantum mechanics
isn't a secure theoretical structure. Hawking, as a relativist, was more con-
cerned with maintaining the theoretical structure of general relativity, so he
was okay with the information being lost if it had to be.
.j^BEfl The reason that this lost information is such a major issue for quantum
' y w\ mechanics once again ties into thermodynamics. In quantum mechanics, infor-
lM|j J mation is related to the thermodynamic concept of "order." If information is
lost, then order is lost — meaning that entropy (disorder) is increased. This
means that the black holes would begin generating heat, rising up to billions
.Chapter 14: Our Universe — String Theory, Cosmology, and Astrophysics 233
of billions of degrees in mere moments. Though Leonard Susskind and others
realized this in the mid-1980s, they couldn't find the flaws in Hawking's reason-
ing that would prove him wrong.
In 2004, after a debate that lasted more than 20 years, Hawking announced
that he no longer believed this information was forever lost to the universe.
In doing so, he lost a 1997 bet with physicist John Preskill. The payoff was a
baseball encyclopedia, from which information could be retrieved easily. And
who said physicists didn't have a sense of humor?
One reason for Hawking's change of mind was that he redid some of his ear-
lier calculations and found that it was possible that, as an object fell into a
black hole, it would disturb the black hole's radiation field. The information
about the object could seep out, though probably in mangled form, through
the fluctuations in this field.
Another way to approach the problem of black hole information loss is
through the holographic principle of Leonard Susskind and Gerard 't Hooft,
or the related AdS/CFT correspondence developed by Juan Maldacena. (Both
of these principles are discussed in Chapter 11.) If these principles hold for
black holes, it may be possible that all the information within the black hole
is also encoded in some form on the surface area of the black hole.
The controversy over the black hole information paradox is described in
detail in Susskind's 2008 book, The Black Hole War: My Battle with Stephen
Hawking to Make the World Safe for Quantum Mechanics.
Still one other approach is to look at the potential multiverse. It's possible that
the information that enters a black hole is, in some way, passed from this uni-
verse into a parallel universe. 1 cover this intriguing possibility in Chapter 15.
The Evolution of the Universe
Other questions that scientists hope string theory can answer involve the way
the universe changes over time. The brane world scenarios described earlier in
this book offer some possibilities, as do the various concepts of a multiverse.
Specifically, string theorists hope to understand the reason for the increased
expansion of our universe as defined by dark matter and energy.
The swelling continues: Eternal inflation
Some cosmologists have worked hard on a theory called eternal inflation,
which helps contribute to the idea of a vast multiverse of possible universes,
each with different laws (or different solutions to the same law, to be precise).
<£j£l Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
In eternal inflation, island universes spring up and disappear throughout the
universe, spawned by the very quantum fluctuations of the vacuum energy
itself. This is seen by many as further evidence for the string theory landscape
and the application of the anthropic principle.
The inflation theory says that our universe began on a hill (or ledge) of poten-
tial vacuum energies. The universe began to roll down that hill rapidly — that
is, our universe began expanding at an exponential rate — until we settled into
a valley of vacuum energy. The question that eternal inflation tries to answer
is: Why did we start on that hill?
Seemingly, the universe started with a random starting point on the spectrum
of possible energies, so it's only luck that we were on the hill and, in turn,
luck that we went through the right amount of inflation to distribute mass
and energy the way it's distributed.
Or, alternately, there are a vast number of possibilities, many of which spring
into existence, and we could only possibly exist in the ones that have this
specific starting condition. (This is, in essence, the anthropic argument.)
In either case, the particles and forces of our universe are determined by the
initial location on that hill and the laws of physics that govern how the uni-
verse will change over time.
In 1977, Sidney Coleman and Frank De Luccia described how quantum fluc-
tuations in an inflating universe create tiny bubbles in the fabric of space-
time. These bubbles can be treated as small universes in their own right (see
Chapter 15). For now, the key is that they do form.
The cosmologist Andrei Linde has been the one to most strenuously argue
that this finding, in combination with Alan Guth's inflationary theory,
demands eternal inflation — the creation of a vast population of universes,
each with slightly different physical properties. He has been joined by Guth
himself and Alexander Vilenkin, who helped hammer out the key aspects of
the theory.
The eternal inflation model says that these bubble universes (Guth prefers
"pocket universes," while Susskind calls them "island universes") spring up,
somehow getting physical laws among the possible ones dictated by the
string theory landscape (through some as-yet-unknown means). The bubble
universe then undergoes inflation. Meanwhile, the space around it continues
to expand — and it expands so quickly that information about the inflating
bubble universe can never reach another universe. Our own universe is one
of these bubble universes, but one which finished its inflationary period
long ago.
.Chapter 14: Our Universe — String Theory, Cosmology, and Astrophysics 233
The hidden matter and energy
Two mysteries of our universe are the dark matter and dark energy (Chapter 9
contains the basics about these concepts). Dark matter is unseen matter that
holds stars together in galaxies, while dark energy is unseen vacuum energy
that pushes different galaxies farther apart from each other. String theory
holds several possibilities for both.
A stringy look at dark matter
String theory provides a natural candidate for dark matter in supersymmetric
particles, which are needed to make the theory work but which scientists
have never observed. Alternatively, it's possible that dark matter somehow
results from the gravitational influence of nearby branes.
Probably the simplest explanation of dark matter would be a vast sea of
supersymmetric particles residing inside galaxies, but we can't see them
(presumably because of some unknown properties of these new particles).
Supersymmetry implies that every particle science knows about has a super-
partner (see Chapter 10 if you need a refresher on supersymmetry). Fermions
have bosonic superpartners and bosons have fermionic superpartners. In
fact, one popular candidate for the missing dark matter is the photino, the
superpartner of the photon.
A computer simulation, reported in the journal Nature in November 2008,
offers one possible means of testing this idea. The simulation, performed
by the international Virgo Consortium research group, suggests that dark
matter in the halo of the Milky Way galaxy should produce detectable levels
of gamma rays. This simulation indicates a direction to start looking for such
tell-tale signs, at least.
Another possible dark matter candidate comes from the various brane world
scenarios. Though the details still have to be worked out, it's possible that
there are branes that overlap with our own 3-brane. Perhaps where we have
galaxies, there are gravitational objects that extend into other branes. Because
gravity is the one force that can interact across the branes, it's possible that
these hyper-dimensional objects create added gravity within our own 3-brane.
Finally, the 4-dimensional string theories discussed in Chapter 13 present yet
another possibility, because they require not only supersymmetry but a vast
number of families of particles beyond the electron, muon, and tau families in
our current Standard Model. Bringing string theory down to four dimensions
seems to greatly expand the number of particles that physicists would expect
to find in the universe, and (if they exist) these could account for dark matter.
A stringy took at dark energy
Even more intriguing than dark matter is dark energy, which is a positive
energy that seems to permeate the entire universe and to be much more
256
Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
abundant than either form of matter — but also much less abundant than
physicists think it should be. Recent discoveries in string theory have allowed
for this dark energy to exist with in the theory.
Although string theory offers some possibilities for dark matter, it offers less
explanation for dark energy. Theoretically, dark energy should be explained
by the value of the vacuum energy in particle physics, where particles
are continually created and destroyed. These quantum fluctuations grow
immensely, leading to infinite values. (I explain in Chapter 8 that to avoid
these infinite values in quantum field theory, the process of renormalization
is used, which is essentially rounding the quantity to a noninfinite value. This
wouldn't be viewed as a favorable method, except for the fact that it works.)
However, when physicists try to use their standard methods to compute the
value of the vacuum energy, they get a value that is off from the experimental
value of dark energy by 10 120 !
The real value is incredibly small, but not quite zero. Though the amount of
dark energy in the universe is vast (according to recent data, it makes up about
73 percent of the universe), the intensity of dark energy is very small — so
small that until 1998, scientists assumed the value was exactly zero.
The existence of dark energy (or a positive cosmological constant, depending
on how you want to look at it) doesn't remove the many solutions of string
theory relating to different possible physical laws. The number of solutions
that include dark energy may be on the order of 10 500 . This dark energy
reflects a positive energy built into the very fabric of the universe, likely
related to the energy of the vacuum itself.
To some, the ekpyrotic universe has a benefit over the inflationary model,
because it offers a reason for why we might observe such a value for dark
energy in our universe: That's the part of the cyclic phase that we're in. At
times in the past, the dark energy may have been stronger, and at times in
the future it may be less. To many others, this reason isn't any more intel-
lectually satisfying than the lack of a reason in other cosmological models. It
still amounts to an accidental coincidence (or an application of the anthropic
principle, as discussed later in this chapter).
Outside of the ekpyrotic universe, there's little explanation for what's going
on. The problem of offsetting the expected vacuum energy by such a large
amount — enough to almost, but not quite, cancel it out — is seen by many
physicists as too much chance to contemplate.
Many would rather turn to the anthropic principle to explain it. Others see
that as waving a white flag of surrender, admitting that dark energy is just too
tough of a challenge to figure out.
Chapter 14: Our Universe — String Theory, Cosmology, and Astrophysics £J /
The Undiscovered Country:
The Future of the Cosmos
In cosmology, the past and the future are linked together, and the expla-
nation for one is tied to the explanation of the other. With the big bang
model in place, there are essentially three possible futures for our universe.
Determining the solutions to string theory that apply to our universe might
allow us to determine which future is most likely.
A universe of ice: The biq freeze
In this model of the universe's future, the universe continues to expand for-
ever. Energy slowly dissipates across a wider and wider volume of space and,
eventually, the result is a vast cold expanse of space as the stars die. This big
freeze has always had some degree of popularity, dating back to the rise of
thermodynamics in the 1800s.
The laws of thermodynamics tell you that the entropy, or disorder, in a
system will always increase. This means that the heat will spread out. In the
context of cosmology, this means that the stars will die and their energy will
radiate outward. In this "heat death," the universe becomes a static soup of
near-absolute zero energy. The universe as a whole reaches a state of ther-
mal equilibrium, meaning that nothing interesting can really happen.
A slightly different version of the big freeze model is based on the more
recent discovery of dark energy. In this case, the repulsive gravity of dark
energy will cause clusters of a galaxy to move apart from each other, while,
on the smaller scale, those clusters will gather closer together, eventually
forming one large galaxy.
Over time, the universe will be populated by large galaxies that are extremely
far apart from each other. The galaxies will become inhospitable to life, and
the other galaxies will be too far away to even see. This variant, sometimes
called a "cold death," is another way the universe could end as a frozen
wasteland. (This timescale is incredibly vast, and humans will likely not even
still exist. So no need to panic.)
From point to point: The big crunch
One model for the future of the universe is that the mass density of the uni-
verse is high enough that the attractive gravity will eventually overpower the
repulsive gravity of dark energy. In this big crunch model, the universe con-
tracts back into a microscopic point of mass.
</f)0 Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
This idea of a big crunch was a popular notion when I was in high school and
reading science fiction, but with the discovery of the repulsive dark energy, it
seems to have gone out of favor. Because physicists are observing the expan-
sion rate increase, it's unlikely that there's enough matter to overcome that
and pull it all back together.
A new beginning: The big bounce
The ekpyrotic model (see the earlier section "A brane-fueled, 21st-century
cyclic model: The ekpyrotic universe") brings the big crunch back, but with
a twist. When the crunch occurs, the universe once again goes through a
big bang period. This is not the only model that allows for such a big bounce
cyclic model.
In the ekpyrotic model, the universe goes through a series of big bangs, fol-
lowed by expansion and then a contracting big crunch. The cycle repeats
over and over, presumably without any beginning or end. Cyclic models of
the universe are not original, going back not only to 1930s physics, but also
to religions, such as some interpretations of Hinduism.
It turns out that string theory's major competitor — loop quantum gravity
(explained in Chapter 18) — may also present a big bounce picture. The
method of loop quantum gravity is to quantize (break up into discrete units)
space-time itself, and this avoids a singularity at the formation of the uni-
verse, which means that it's possible that time extends back before the big
bang moment. In such a picture, a big bounce scenario is likely.
Exploring a Finely. Tuned Universe
One major issue in cosmology for years has been the apparent fine-tuning
seen in our universe. The universe seems specially crafted to allow life. One
of the major explanations for this is the anthropic principle, which many
string theorists have recently begun adopting. Many physicists still feel that
the anthropic principle is a poor substitute for an explanation of why these
physical properties must have the values they do.
To a physicist, the universe looks as if it were made for the creation of life.
British Astronomer Royal Martin Rees clearly illuminated this situation in
his 1999 book Just Six Numbers: The Deep Forces That Shape the Universe. In
this book, Rees points out that there are many values — the intensity of dark
energy, gravity, electromagnetic forces, atomic binding energies, to name just
a few — that would, if different by even an extremely small amount, result
.Chapter 14: Our Universe — String Theory, Cosmology, and Astrophysics 25 y
in a universe that is inhospitable to life as we know it. (In some cases, the
universe would have collapsed only moments after creation, resulting in a
universe inhospitable for any form of life.)
The goal of science has always been to explain why nature has to have these
values. This idea was once posed by Einstein's famous question: Did God
have a choice in creating the universe?
Einstein's religious views are complex, but what he meant by this question
wasn't actually so much religious as scientific. In other words, he was wonder-
ing if there was a fundamental reason — buried in the laws of nature — why
the universe turned out the way it did.
For years, scientists sought to explain the way the universe worked in terms of
fundamental principles that dictate the way the universe has formed. However,
with string theory (and eternal inflation), that very process has resulted in
answers that imply the existence of a vast number of universes and a vast
number of scientific laws, which could be applied in those universes.
The major success of the anthropic principle is that it provided one of the
only predictions for a small, but positive, cosmological constant prior to
the discovery of dark energy. This was put forward in the 1986 book The
Anthropic Cosmological Principle by John D. Barrow and Frank J. Tipler, and
cosmologists in the 1980s appeared to be at least open-minded about the
possibility of using anthropic reasoning.
Nobel laureate Steven Weinberg made the big case for anthropic reasoning in
1987. Analyzing details of how the universe formed, he realized two things:
11^ If the cosmological constant were negative, the universe would quickly
collapse.
V If the cosmological constant were slightly larger than the experimentally
possible value, matter would have been pushed apart too quickly for gal-
axies to form.
In other words, Weinberg realized that if scientists based their analysis on
what was required to make life possible, then the cosmological constant
couldn't be negative and had to be very small. There was no reason, in his
analysis, for it to be exactly zero. A little over a decade later, astronomers
discovered dark energy, which fit the cosmological constant in precisely the
range specified by Weinberg. Martin Rees appealed to this type of discovery
in his explanation of how the laws in our universe end up with such finely
tuned values, including the cosmological constant.
260
Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
You may wonder if there's anything particularly anthropic about Weinberg's
reasoning, however. You only have to look around to realize that the uni-
verse didn't collapse and galaxies were able to form. It seems like this argu-
ment could be made just by observation.
The problem is that physicists are looking not only to determine the proper-
ties of our universe, but to explain them. To use this reasoning to explain the
special status of our universe (that is, it contains us) requires something very
important — a large number of other universes, most of which have proper-
ties that make them significantly different from us.
For an analogy, consider you're driving along and get a flat tire. If you were the
only person who had ever gotten a flat tire, you might be tempted to explain
the reason why you, out of everyone on the planet, were the one to get the flat
tire. Knowing that many people get flat tires every day, no further explanation
is needed — you just happen to have been in one of many cars that happened
to get a flat tire.
If there is only one universe, then having the fine-tuned numbers that Rees
and others note is a miraculously fortunate turn of events. If there are billions
of universes, each with random laws from hundreds of billions (or more) pos-
sible laws from the string theory landscape, then every once in a while a uni-
verse like ours will be created. No further explanation is necessary.
The problem with the anthropic principle is that it tends to be a last resort for
physicists. Scientists only turn to the anthropic principle when more conven-
tional methods of arguments have failed them, and the second they can come
up with a different explanation, they abandon it.
This isn't to imply that the scientists applying the anthropic principle are
anything but sincere. Those who adopt it seem to believe that the vast string
theory landscape — realized in a multiverse of possible universes (see
Chapter 15) — can be used to explain the properties of our universe.
Chapter 15
Parallel Universes: Maybe You
Can Be Two Places at Once
In This Chapter
Examining the four types of parallel universes
Using holes and tunnels to check out other universes
Explaining our universe by our presence
c
^ktring theory and its infant sibling, string cosmology, certainly give us
^r amazing possibilities for what could be out there in our universe, but
they also give us even more amazing possibilities about what could be out
there beyond our universe, in other universes that may or may not have any
connection with ours.
In this chapter, I explain what science in general, and string theory in particu-
lar, has to tell us about the possible existence of alternate universes. I start
with a general discussion of these different types of parallel universes and
then get into the specific traits of each. I also take a brief look at how quan-
tum physics could possibly provide a way for intelligent beings from one uni-
verse to possibly contact another universe. Finally, the anthropic principle
comes up again, and I explain how it relates to the ideas of parallel universes.
Exploring the Multiverse: A Theory
of Parallel Universes
The multiverse is a theory in which our universe is not the only one, but
states that many universes exist parallel to each other. These distinct uni-
verses within the multiverse theory are called parallel universes. A variety of
different theories lend themselves to a multiverse viewpoint.
262
Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
Multiverses in religion and philosophy
The idea of a physical multiverse came later to
physics than in some other areas. The Hindu
religion has ancient concepts that are similar.
The term itself was, apparently, first applied by
a psychologist, rather than a physicist.
Concepts of a multiverse are evident in the
cyclical infinite worlds of ancient Hindu cos-
mology. In this viewpoint, our world is one of
an infinite number of distinct worlds, each gov-
erned by its own gods on their own cycles of
creation and destruction.
The word multiverse was originated by
American psychologist William James in 1895
(the word "moral" is excluded from some cita-
tions of this passage):
"Visible nature is all plasticity and indiffer-
ence, a [moral] multiverse, as one might
call it, and not a [moral] universe."
The phrase rose in prominence throughout the
20th century, when it was used regularly in sci-
ence fiction and fantasy, notably in the work
of author Michael Moorcock (though some
sources attribute the word to the earlier work
of author and philosopher John Cowper Powys
in the 1950s). It is now a common phrase within
these genres.
In some theories, there are copies of you sitting right here right now read-
ing this book in other universes and other copies of you that are doing other
things in other universes. Other theories contain parallel universes that are so
radically different from our own that they follow entirely different fundamental
laws of physics (or at least the same laws manifest in fundamentally different
ways), likely collapsing or expanding so quickly that life never develops.
Not all physicists really believe that these universes exist. Even fewer believe
that it would ever be possible to contact these parallel universes, likely not
even in the entire span of our universe's history. Others believe the quan-
tum physics adage that if it's possible, it's bound to happen somewhere and
sometime, meaning it may be inevitable that quantum effects allow contact
between parallel universes.
According to MIT cosmologist Max Tegmark, there are four levels of parallel
universes:
u* Level 1: An infinite universe that, by the laws of probability, must con-
tain another copy of Earth somewhere
v" Level 2: Other distant regions of space with different physical param-
eters, but the same basic laws
u* Level 3: Other universes where each possibility that can exist does
exist, as described by the many worlds interpretation (MWI) of quantum
physics
.Chapter 15: Parallel Universes: Maybe You Can Be Two Places at Once 20 J
Iv* Level 4: Entirely distinct universes that may not even be connected to
ours in any meaningful way and very likely have entirely different funda-
mental physical laws
The following sections look at each of these levels in more detail.
Tegmark's approach is one of the only attempts to comprehensively catego-
rize the concepts of parallel universes in a scientific (or, as some see it, pseu-
doscientific) context. The full text of Tegmark's 2003 paper on this
topic is available at his MIT Web site, space .mit . edu/home/tegmark/
multiverse . pdf , for those who don't believe that these concepts are sci-
entific. (They may not be scientific, but if that's the case, then at least they're
unscientific musings by a scientist.)
Plurality of worlds: A hot topic
Early astronomy provided some support for
the existence of a plurality of worlds, a view
that was so controversial that it contributed
to at least one man's death. These plurality of
worlds, and the eventual parallel worlds, were
rooted in the ideas of an infinite universe, as are
the ideas of parallel universes presented in this
chapter.
The Italian philosopher Giordano Bruno ( 1 548—
1600) was executed for a variety of heresies
against the Catholic Church. Though Bruno
was a supporter of the Copernican system,
his abnormal beliefs went far beyond that: He
believed in an eternal and infinite universe
that contained a plurality of worlds. Bruno rea-
soned that because God was infinite, his cre-
ation would similarly be infinite. Each star was
another sun, like our own, about which other
worlds revolved. He didn't feel that such view-
points were in opposition to the scriptures.
In fairness to the Catholic Church, Bruno
wasn't executed merely for believing in other
worlds. His list of heresies was long and varied,
including denial of Mary's virginity, the divinity
of Christ, the Trinity, the Incarnation, and the
Catholic doctrine of transubstantiation. He also
believed in reincarnation and was accused of
practicing magic. This is not to say that any (or
all) of these viewpoints warranted death, but
given the time period, it would be hard to get
out of such accusations alive.
In 1686, the French writer Bernard le Bovier de
Fontenelle wrote Conversations on the Plurality
of Worlds, which was one of the first books
to address the popular audience on scientific
topics, being written in French rather than
scholarly Latin. In Conversations, he explained
the Copernican heliocentric model of the uni-
verse and contemplated extraterrestrial life.
Though other enlightenment thinkers — pos-
sibly even John Adams and Benjamin Franklin,
by some accounts — were agreeable to such
viewpoints, it would be many years before the
plurality of worlds extended to the plurality of
universes.
In 1871, the French political malcontent
Louis Auguste Blanqui wrote — while in
prison — a brochure titled Eternity by the Stars:
Astronomical Hypotheses, in which he said that
an infinite universe would have to replicate the
original set of combinations an infinite number
of times to fill up the infinite space. This is, to
my knowledge, the first inkling of the transition
from "plurality of worlds" to "parallel worlds" —
copies of you sitting reading this same book on
another planet.
4m\)ll Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
LeVel 1: If you go far enough,
you'll get back home
The idea of Level 1 parallel universes basically says that space is so big that
the rules of probability imply that surely, somewhere else out there, are
other planets exactly like Earth. In fact, an infinite universe would have infi-
nitely many planets, and on some of them, the events that play out would be
virtually identical to those on our own Earth.
We don't see these other universes because our cosmic vision is limited by
the speed of light — the ultimate speed limit. Light started traveling at the
moment of the big bang, about 14 billion years ago, and so we can't see any
further than about 14 billion light-years (a bit farther, since space is expand-
ing). This volume of space is called the Hubble volume and represents our
observable universe.
The existence of Level 1 parallel universes depends on two assumptions:
V The universe is infinite (or virtually so).
j-" Within an infinite universe, every single possible configuration of par-
ticles in a Hubble volume takes place multiple times.
In regard to the first assumption, inflation theory predicts that the universe
is actually far larger than our Hubble volume. Recall that eternal inflation
implies that universes are constantly being created and destroyed by quan-
tum fluctuations, which means that space is actually infinite under the most
extreme application of this theory.
The regions created in an eternal inflation model trigger every single set of
initial conditions, leading to the second assumption. This means that there's
another region of space that consists of a Hubble volume that has the exact
same initial conditions as our universe. If it has exactly the same initial condi-
tions, then such a region would evolve into a Hubble volume that resembles
ours exactly.
If Level 1 parallel universes do exist, reaching one is virtually (but not
entirely) impossible. For one thing, we wouldn't know where to look for one
because, by definition, a Level 1 parallel universe is so far away that no mes-
sage can ever get from us to them, or them to us. (Remember, we can only
get messages from within our own Hubble volume.)
In theory, however, you could get in a spaceship that can travel at nearly
the speed of light, point it in a direction, and head off. Time for you would
slow, but the universe would continue to age as you moved throughout the
entire expanse of the universe looking for your twin. If you're lucky, and dark
energy is weak enough that eventually gravity causes cosmic expansion to
end, you might eventually be able to get to your twin's planet.
.Chapter 15: Parallel Universes: Maybe You Can Be Two Places at Once
265
Chaotic and eternal: Two facets of inflation
The theories of eternal inflation and chaotic
inflation can be quite confusing, as I discovered
in writing this book. Most people, even physi-
cists, use them fairly interchangeably. This is
an excellent example of how concepts on the
cutting edge of science can get blurred, even
between different experts in the field.
In eternal inflation, the quantum fluctuations in
the vacuum energy result in "bubble universes"
(or "pocket universes" or "island universes" . . .
will the naming confusion never cease?!). The
possible energies that such a universe could
have (called the false vacuum) are represented
by a graph that looks kind of like a mountain
range, which is often referred to as an energy
hill. The true vacuum of our universe is repre-
sented as one of the valleys in such a graph.
In 1983, Paul Steinhardt and Alex Vilenkin both
presented the key ideas of eternal inflation,
which is that quantum fluctuations can cause
the triggering of new inflationary cycles. The
assumption at the time was that each new
cycle of inflation would start at the top of the
energy hill and, during the inflationary cycle,
would progress down toward the true vacuum.
The energy state of the universe is decaying
into a ground state.
In
Andrei Linde wrote a paper called
Chaotic Inflation," in which he pointed out that
these universes can be created anywhere on
the energy hill, not necessarily at the peak. In
fact, the hill itself may not even have a peak;
it might continue on forever! He furthermore
showed that chaotic inflation is also eternal,
because it spawns continued creation of new
bubble universes.
Several sources make chaotic inflation sound
like a specific type of eternal inflation theory.
Max Tegmark's 2003 article uses "chaotic
inflation" in a way that sounds, to me, more like
eternal inflation. Wikipedia has an article on
chaotic inflation, identifying it as a "sub-class
of eternal inflation," but has no article on eter-
nal inflation itself!
But Vilenkin, in his 2006 book, Many Worlds in
One: The Search for Other Universes, is ada-
mant that chaotic inflation is an entirely differ-
ent theory, seeming a bit frustrated that they're
so often interchanged, a frustration that cer-
tainly seems justified, unless Vilenkin is the one
who's applying the term imprecisely.
Time will tell what consensus cosmologists
reach over this distinction between chaotic
inflation and eternal inflation. For now, though,
it's useful to know that most chaotic models will
yield eternal inflation (but not all of them), and
many eternal inflation models are not chaotic.
LeVel 2: If you go far enough,
you'll fall into Wonderland
In a Level 2 parallel universe, regions of space are continuing to undergo an
inflation phase. Because of the continuing inflationary phase in these uni-
verses, space between us and the other universes is literally expanding faster
than the speed of light — and they are, therefore, completely unreachable.
266
Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
Two possible theories present reasons to believe that Level 2 parallel uni-
verses may exist: eternal inflation and ekpyrotic theory. Both theories were
introduced in Chapter 14, but now you can see one of the consequences in
action.
In eternal inflation, recall that the quantum fluctuations in the early uni-
verse's vacuum energy caused bubble universes to be created all over the
place, expanding through their inflation stages at different rates. The initial
condition of these universes is assumed to be at a maximum energy level,
although at least one variant, chaotic inflation, predicts that the initial condi-
tion can be chaotically chosen as any energy level, which may have no maxi-
mum, and the results will be the same. (See the nearby sidebar "Chaotic and
eternal: Two facets of inflation" for more information.)
The findings of eternal inflation mean that when inflation starts, it produces
not just one universe, but an infinite number of universes.
Right now, the only noninflationary model that carries any kind of weight
is the ekpyrotic model, which is so new that it's still highly speculative.
(Ironically, both the eternal inflation model and the ekpyrotic model were
partially created by cosmologist Paul Steinhardt.)
In the ekpyrotic theory picture, if the universe is the region that results when
two branes collide, then the branes could actually collide in multiple loca-
tions. Consider flapping a sheet up and down rapidly onto the surface of a
bed. The sheet doesn't touch the bed only in one location, but rather touches
it in multiple locations. If the sheet were a brane, then each point of collision
would create its own universe with its own initial conditions.
There's no reason to expect that branes collide in only one place, so the
ekpyrotic theory makes it very probable that there are other universes in
other locations, expanding even as you consider this possibility.
In other words, modern cosmology — regardless of whether inflation or ekpy-
rosis are true — virtually demands that Level 2 parallel universes exist. (Some
alternate cosmological theories presented in Chapter 19, such as variable
speed of light cosmology and modified gravity, don't have this demand.)
As in the Level 1 universes, these universes would be created with essentially
random initial conditions, which, averaged out over infinity, implies that
there are other universes that are virtually (or completely) identical to our
own. These new universes are continually formed, so many (infinitely many,
in fact) are still undergoing the inflationary phase of their evolution.
Unlike in a Level 1 universe, it's possible that a Level 2 universe could have
different fundamental properties, such as a higher (or lower) number of
dimensions, a different array of elementary particles, fundamental force
.Chapter 15: Parallel Universes: Maybe You Can Be Two Places at Once J? /
strengths, and so on. But these universes are created by the same laws of
physics that created ours, just with different parameters. These universes
could behave quite differently from our own, but the laws that govern them
would — on a very fundamental level — be exactly the same.
Unfortunately, Level 2 universes are pretty much impossible to reach. Not
only are there an infinite number of universes, but there are an infinite
number of inflating universes, which means the space between our universe
and a parallel universe is expanding. So even if we could move at the speed
of light (and we can't), we'd never be able to get to another universe. Space
itself is inflating faster than we can move between our universe and another
Level 2 universe.
LeVel 3: If you stay where you
are, you'll run into yourself
A Level 3 parallel universe is a consequence of the many worlds interpre-
tation (MWI) from quantum physics. In this interpretation, every single
quantum possibility inherent in the quantum wavefunction becomes a real
possibility in some reality. When the average person (especially a science
fiction fan) thinks of a "parallel universe," he's probably thinking of Level 3
;1 universes.
The many worlds interpretation was presented by Hugh Everett III to explain
the quantum wavefunction, the Schrodinger equation. The Schrodinger equa-
tion describes how a quantum system evolves over time through a series of
rotations in a Hilbert space (an abstract space with infinite dimensions). The
evolution of the wavefunction is called unitary. (Unitarity basically means
that if you add up the probabilities of all possible outcomes, you get 1 as the
sum of those probabilities.)
The traditional Copenhagen interpretation of quantum physics assumed that
the wavefunction collapsed into a specific state, but the theory presented no
mechanism for when or how this collapse takes place. The collapse turned
the unitary wavefunction, which contains all possibilities, into a non-unitary
system, which ignores the possibilities that never took place.
Everett took a tactic similar to that taken later by string theorists, assum-
ing that each "dimension" predicted mathematically by the wavefunction
(an infinite number of them) must be realized in some way in reality. In this
theory, all quantum events result in a branching of a universe into multiple
universes, so the unitary theory can be treated in a unitary way (no possibili-
ties ever go away).
268
Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
Alternate history across many worlds
Of all the types of parallel universes. Level 3
universes have most captured the imagination
of popular culture, spawning their own genre
of science fiction and fantasy: alternate his-
tory. These are stories written with settings
that are based on our own universe, but with
the assumption that some historical eventwent
differently, resulting in consequences different
from those in our own universe. (For the non-
science fiction fan, think of It's a Wonderful
Life.) In these fictional universes, it's possible
(and common) that visitors from one universe
can interact with a Level 3 parallel universe.
Obviously, in these fictional universes, the
author (and reader) care about the macroscopic
differences, but the many worlds interpretation
applies to all levels. If a particle decays, or not,
differentworlds represent those events. No one
observing would be able to tell the difference
between them. However, if they were observing
with a Geiger counter, which detects radioac-
tive decay, the quantum split would result in
further splits. The Geiger counter is triggered
in one universe and not the other. The scientist
who detects the decay would react differently,
perhaps, than the one who does not detect the
decay. So, in principle, this is how these tiny
quantum universes become full-fledged paral-
lel universes.
In fiction, the effects are generally more dra-
matic, such as the southern states winning the
American Civil War or the Byzantine Empire
never collapsing (both of which have been
explored by alternate history author Harry
Turtledove, called "the Master of Alternate
History" by his fans).
Level 3 parallel universes are different from the others posed because they
take place in the same space and time as our own universe, but you still have
no way to access them. You have never had and will never have contact with
any Level 1 or Level 2 universe (I assume), but you're continually in contact
with Level 3 universes — every moment of your life, every decision you
make, is causing a split of your "now" self into an infinite number of future
selves, all of which are unaware of each other.
Though we talk of the universe "splitting," this isn't precisely true (under
the MWI of quantum physics). From a mathematical standpoint, there's only
one wavefunction, and it evolves over time. The superpositions of different
universes all coexist simultaneously in the same infinite-dimensional Hilbert
space. These separate, coexisting universes interfere with each other, yielding
the bizarre quantum behaviors, such as those of the double slit experiment in
Chapter 7.
Of the four types of universes, Level 3 parallel universes have the least to do
with string theory directly.
.Chapter 15: Parallel Universes: Maybe You Can Be Two Places at Once 2vy
LeVel b: Somewhere oVer the rainbow,
there's a magical land
A Level 4 parallel universe is the strangest place (and most controversial pre-
diction) of all, because it would follow fundamentally different mathematical
laws of nature than our universe. In short, any universe that physicists can
get to work out on paper would exist, based on the mathematical democracy
principle: Any universe that is mathematically possible has equal possibility
of actually existing.
Scientists use mathematics as their primary tool to express the theories of
how nature behaves. In a sense, the mathematics that represents the theory
is the meat of the theory, the thing that really gives it substance.
In 1960, physicist Eugene Wigner published an article with the provocative
title "The Unreasonable Effectiveness of Mathematics in the Natural Sciences,"
in which he pointed out that it's kind of unreasonable that mathematics — a
construct purely of the mind — would be so good at describing physical laws.
He went further than this, supposing that this effectiveness represented a deep
level of connection between mathematics and physics, and that by exploring
mathematics you can figure out ways to approach sciences in new and innova-
tive ways.
But the equations that work so well to describe our universe are only one set
of equations. Certainly a universe could be created, as physicists have done
on paper, with only two dimensions and containing no matter, which is noth-
ing but expanding space. There could be a vast anti-de Sitter space, contract-
ing, right next to it.
Why, then, do we observe the specific set of equations, specific set of laws,
that we do? In other words, to use the phrase of British cosmologist Stephen
Hawking (from his 1988.4 Brief History of Time}, what is the force that
"breathes fire into the equations" that govern our universe?
Throughout this book, you explore concepts that are on the cutting edge of
theoretical physics — the bosonic string theory, the various superstring the-
ories, AdS/CFT correspondence, Randall-Sundrum models — but that clearly
don't match our own universe. Most physicists leave it at that, with the
understanding that some "pure math" just doesn't apply directly to the physi-
cal universe we live in. However, according to the principle of mathematical
democracy, these universes do exist somewhere.
2 / i) Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
$HBE# In this controversial view, our equations aren't preferred, but in the multi-
, ^^ffi\ verse, every equation that can have life breathed into it will. This makes up
iMJj ) the Level 4 multiverse, a place so vast and strange that even the most brilliant
among us can only conceptualize it with the tools of mathematics.
Accessing Other Universes
With the four types of parallel universe described, it's time to look at the fun
part — whether there's any way to reach them. Realistically, the answer is
probably "No," but that's not the most interesting option, so the following
sections look into ways that some of these universes might be able to inter-
act with our own.
A history of hyperspace
To access a Level 1, 2, or 4 universe, you'd have to find a way to traverse an
incredibly large distance in a moment's time, a task made more difficult by
Einstein's speed limit — the speed of light. One of the only ways to achieve this
would be by using extra space dimensions — sometimes called hyperspace —
to cut down the distance.
Where are those extra dimensions, anyuray?
Current string theory models postulate ten space dimensions (plus one time
dimension). Our observed universe appears to have only three space dimen-
sions (plus the one time dimension). String theory offers two possibilities for
the extra dimensions:
IJ-" The extra seven dimensions extend off of a 3-brane on which our uni-
verse resides.
u* The extra seven dimensions are compactified (likely into a Planck length
radius shape), while our three space dimensions are uncompactified.
(This is the dominant string theory viewpoint.)
You can picture a modified version of the first possibility by looking at
Figure 15-1, which shows a universe of people living on a 2-brane. A third
dimension extends off of that brane.
In theory, there could be some means for the 2-brane residents to leave the
2-brane and experience the greater 3-dimensional reality, as in the classic
novel Flatland. By extension, there could be a way for people in our universe
to leave our 3-brane to travel in the extra dimensions.
.Chapter 15: Parallel Universes: Maybe You Can Be Two Places at Once 2/1
For the second possibility, the dimensions are compactified to sizes that are
so small no one has ever observed them. As discussed in Chapter 11, some
recent theories have indicated that these sizes could be as large as a visible
fraction of a millimeter, and tests along these lines should take place at the
Large Hadron Collider. Some speculative ideas (not even well developed
enough to be called theories) have been put forth that these compactified
dimensions could contain their own universes.
String theory also allows for the possibility that some regions of the universe
would have large extra dimensions, allowing them to interact with the cur-
rent three dimensions in meaningful ways. No models suggest that this is
actually happening in our universe, but the theory allows for such behavior.
Wormholes: Busting out of three-space
Even before string theory, the idea existed that the geometry of the universe
would allow for shorter paths between points. In fiction, this can be seen in
stories such as Lewis Carroll's Alice in Wonderland, and in science, it can be
seen in the wormholes, as depicted in Figure 1-4 in Chapter 1.
A wormhole is a shortcut to go from one location on a surface to another,
just as a worm can dig through the center of an apple to get from one surface
to another (thus the name). This concept arises from Einstein's theory of
general relativity, proposed years before string theory was conceived. These
traditional wormholes connect different regions in the same universe and, as
you can see in Chapter 16, have been exploited for many outlandish theoreti-
cal purposes, despite the fact that no one knows for sure whether they exist.
(So what's one more!)
J? / 2 P art IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
Similarly, it's possible that in a brane world scenario, we are somehow touch-
ing or connected to another brane. If these branes overlap, it's conceivable
that there would be a way to travel from the space of one brane to the space
of another brane. (This is not the standard way that multiple branes interact
in string theory. Much more common are the brane world scenarios from
Chapter 11, where separate branes host difference pieces of the physics of
our universe and then interact gravitationally.)
It's unlikely that such a brane jump would take place merely by stepping into
a mirror, but something as powerful as a wormhole might do the trick. It's
possible that a wormhole — generally hypothesized by general relativity as
existing within rotating black holes and being notoriously unstable — might
allow bits of matter or energy to slip from one universe into another parallel
universe. If such strange events occurred at points where different branes
overlapped in the bulk (the greater space that contains all of the branes), it's
unclear whether they might provide a way to get matter and energy from one
brane to another as well.
In fact, one possible resolution to the black hole information paradox that
has long been considered by some is the idea that information that enters a
black hole exits into a parallel universe by means of a wormhole at the center
of the black hole.
Such ideas are obviously highly speculative, but mathematical models have
shown it's feasible that some sort of wormhole — if held open by a form of
negative energy — could provide a means of connecting different portions
of space.
If this is the case, then the arguments in favor of parallel universes are on our
side, because given an infinite universe and infinite time, everything is bound
to happen somewhere. In a universe where parallel universes exist, travel
between them may be guaranteed.
How quantum mechanics can
act us from here to there
One other process of getting from one universe to another would be to use
the property of quantum tunneling, which is where a particle is allowed to
"jump" from one location to another across a barrier.
As Chapter 7 reveals, the uncertainty principle of quantum physics means
that particles don't have a definite location, but instead both the location and
momentum of each particle are linked together with a sort of "fuzziness." The
more precisely you determine the location, the more fuzzy the momentum is,
and vice versa.
.Chapter 15: Parallel Universes: Maybe You Can Be Two Places at Once 2 #3
This principle results in a strange phenomenon, known as quantum tunneling
and shown in Figure 15-2. In this case, there is some sort of barrier (usually
a potential energy barrier) that the particle shouldn't be able to cross nor-
mally. But the graph, which represents the probability that the particle is in
any given location, extends a bit across the barrier.
Figure 15-2:
According
to quantum
physics,
sometimes
particles
can
"tunnel"
across
barriers.
Probability that
particles will "tunnel"
In other words, even when there's an uncrossable barrier, there's a slight
chance — according to quantum mechanics — that a particle that should be
on one side of the barrier may end up on the other side of the barrier. This
behavior has been confirmed by experiment.
This provides a means that could in theory be used to access a parallel uni-
verse. Some cosmologists have suggested that exactly this physical mecha-
nism is what started our own expansion as a universe.
The idea of quantum tunneling is key to the operation of electron-tunneling
microscopes, which allow scientists to observe objects in incredibly fine
detail.
Particles can only tunnel from a higher energy state into a lower energy state,
though, so there are some limits on how this could be used, and the idea of
using it to access another universe in a controlled way is way beyond current
technology (or even current theory).
But for a sufficiently advanced civilization, one that has a theory that fully
explains all aspects of physics and the ability to use vast amounts of energy,
this sort of idea may be a possible means of getting to another universe.
2 / 11 Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
Eaten by rogue universes
The assumption in this chapter has mostly
been that the separate universes described
don't normally interact with each other, but
some approaches over the years have called
this into question. One of the most recent is
a 2008 paper in the journal Physics Review D
by Eduardo Guendelman and Nobuyuki Sakai,
in which they examine the idea of bubble uni-
verses to see if they could expand without the
need for a big bang.
To make the equations work, Guendelman and
Sakai had to introduce a repulsive phantom
energy, which is possibly similar to dark energy.
They found two types of stable solutions:
u* The child universe, which is isolated from
the parent universe (essentially a universe
inside a black hole)
»-" A rogue universe, which is not isolated from
the parent universe
This second kind of universe is troublesome,
because as it begins to go through its inflation
cycle, it does so by devouring the space-time
of the parent universe. The parent universe is
swept away as the rogue universe expands in
its place — and it does so faster than the speed
of light, so there's no warning.
Fortunately, there's no evidence that this phan-
tom energy actually exists, or, if it does, it's pos-
sible that it exists in the form of dark energy (or
inflation energy), which means that we may be
one of these rogue universes ourselves. As our
universe expands, it may be devouring some
other, larger universe!
Chapter 16
Have Time, Will Travel
In This Chapter
Scientists are still trying to figure out why we travel through time
Tricking time with relativity
Need more time? Considering the possibility of a second time dimension
Logical paradoxes: The fun part of time travel
■ Mne of the most fascinating concepts in science fiction is the idea of trav-
^^ eling forward or backward in time, as in H. G. Wells's classic story The
Time Machine. Scientists haven't been able to build a time machine yet, but
some physicists believe that it may someday be possible — and some (prob-
ably most) believe that it will never be possible.
Time travel exists in physics because of possible solutions to Einstein's gen-
eral theory of relativity, mostly resulting in singularities. These singularities
would be eliminated by string theory, so in a universe where string theory
dictates the laws of the universe, time travel will probably not be allowed —
a result that many physicists find quite favorable to the alternative (though
far less interesting).
In this chapter, I explore the notion of time and our travel through it — both
in the normal, day-to-day method and in more unusual, speculative methods.
I discuss the scientific meaning of time, in both classical terms and from the
standpoint of special relativity. One possible method of time travel involves
using cosmic strings. There's a possibility, which I explore, that there may
be more than one time dimension. I also explain one scenario for creating a
physically plausible (though probably impossible) time machine using worm-
holes. Finally, I look at some of the different logical paradoxes involved with
time travel.
276
Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
Temporal Mechanics 101:
Hou/ Time Flies
We move through time every single day, and most of us don't even think
about how fascinating it is. Scientists who have thought about it have con-
stantly run into trouble in figuring out exactly what time means because time
is such an abstract concept. It's something we're intimately familiar with, but
so familiar with that we almost never have to analyze it in a meaningful way.
Over the years, our view of time — both individually and from a scientific
standpoint — has changed dramatically, from an intuition about the passage
of events to a fundamental component of the mathematical geometry that
describes the universe.
The arrow of time: A one-Way ticket
Physicists refer to the one-way motion through time (into the future and never
the past) using the phrase "arrow of time," first used by Arthur Eddington
(the guy who helped confirm general relativity) in his 1928 book The Nature
of the Physical World. The first note he makes is that "time's arrow" points in
one direction, as opposed to directions in space, where you can reorient as
needed. He then points out three key ideas about the arrow of time:
U* Human consciousness inherently recognizes the direction of time.
e* Even without memory, the world only makes sense if the arrow of time
points into the future.
J-" In physics, the only place the direction of time shows up is in the
behavior of a large number of particles, in the form of the second law
of thermodynamics. (See the nearby sidebar, "Time asymmetries," for a
clarification of the exceptions to this.)
The conscious recognition of time is the first (and most significant) evidence
that any of us has about the direction we travel in time. Our minds (along
with the rest of us) "move" sequentially in one direction through time, and
most definitely not in the other. The neural pathways form in our brain,
which retains this record of events. In our minds, the past and future are
distinctly different. The past is static and unchanging, but the future is fully
undetermined (at least so far as our brain knows).
As Eddington pointed out, even if you didn't retain any sort of memory, logic
would dictate that the past must have happened before the future. This is
probably true, although whether one could conceptualize of a universe in
which time flowed from the future to the past is a question that's open for
debate.
.Chapter 16: Have Time, Will Travel 277
Time asymmetries
Arthur Eddington's third observation about
the arrow of time indicates that physical laws
actually ignore the direction of time, except
for the second law of thermodynamics. What
this means is that if you take the time fin any
physics equation and replace it with a time -t,
and then perform the calculations to describe
what takes place, you'll end up with a resultthat
makes sense.
For gravity, electromagnetism, and the strong
nuclear force, changing the sign on the time
variable (called T-symmetry) allows the laws of
physics to work perfectly well. In some special
cases related to the weak nuclear force, this
actually turns out not to be the case.
There is actually a largertype of symmetry, called
CPT symmetry, which is always preserved. The C
stands for charge-conjugation symmetry, which
means that positive and negative charges switch.
The P stands for parity symmetry, which involves
basically replacing a particle for a complete
mirror image — a particle that has been flipped
across all three space dimensions. (This CPT
symmetry is a property of quantum theory in our
four-dimensional space-time, so at present we
are ignoring the other six dimensions proposed
by string theory.)
The total CPT symmetry, it turns out, appears to
be preserved in nature. (This is one of the few
cases of unbroken symmetry in our universe.)
In other words, an exact mirror image of our
universe — one with all matter swapped for
antimatter, reflected in all spatial directions,
and traveling backward in time — would obey
physical laws that are identical to those of our
own universe in every conceivable way.
If CP symmetry is violated, then there must be a
corresponding break in T-symmetry, so the total
CPT symmetry is preserved. In fact, the handful
of processes that violate T-symmetry are called
CPi//o/af/o/7s(becausethe CP violation is easier
to test than a violation in the time-reversal
symmetry).
Finally, though, we reach the physics of the situation: the second law of
thermodynamics. According to this law, as time progresses, no closed system
(that is, a system that isn't gaining energy from outside of the system) can
lose entropy (disorder) as time progresses. In other words, as time goes on,
it's not possible for a closed system to become more orderly.
Intuitively, this is certainly the case. If you look at a house that's been aban-
doned, it will grow disordered over time. For it to become more orderly, there
has to be an introduction of work from outside the system. Someone has to
mow the yard, clean the gutters, paint the walls, and so on. (This analogy isn't
perfect, because even the abandoned house gets energy and influence from
outside — sunlight, animals, rainfall, and so on — but you get the idea.)
In physics, the arrow in time is the direction in which entropy (disorder)
increases. It's the direction of decay.
2 / O Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
Oddly, these same ideas (the same in spirit, though not scientific) date all
the way back to St. Augustine of Alexandria's Confessions, written in 400 BCE,
where he said:
"What then is time? If no one asks me, I know: if I wish to explain it to one
that asketh, I know not: yet I say boldly that I know, that if nothing passed
away, time were not; and if nothing were, time present were not."
What Augustine is pointing out here is the inherent problem in explaining
the slippery nature of time. We know exactly what time is — in fact, we are
unable not to understand how it flows in our own lives — but when we try to
define it in precise terms, it eludes us. He speaks of "if nothing passed away,
time were not" that could, in a sense, describe how the second law of thermo-
dynamics defines time's arrow. We know time passes because things change
in a certain way as time passes.
Relativity, Worldlines, and Worldsheets:
Moving through space-time
Understanding how time travel works within string theory would require a
complete understanding of how the fabric of space-time behaves within the
theory. So far, string theory hasn't exactly figured that out.
In general relativity, the motion of objects through space-time is described
by a worldline. In string theory, scientists talk about strings (and branes) cre-
ating entire worldsheets as they move through space-time.
Worldlines were originally constructed by Hermann Minkowski when he cre-
ated his Minkowski diagrams, shown in Chapter 6. Similar diagrams return
in the form of Feynman diagrams (see Chapter 8), which demonstrate the
worldlines of particles as they interact with each other through the exchange
of gauge bosons.
In string theory, instead of the straight worldlines of point particles, it is the
movement of strings through space-time that interests scientists, as shown in
the right side of Figure 16-1.
Notice that in the original Feynman diagram, shown on the left of Figure 16-1,
there are sharp points where the worldlines intersect (representing the point
where the particles interact). In the worldsheet, the virtual string exchanged
between the two original strings creates a smooth curve that has no sharp
points. This equates to the fact that string theory contains no infinities in
the description of this interaction, as opposed to pure quantum field theory.
(Removing the infinities in quantum field theory requires renormalization.)
.Chapter 16: Have Time, Will Travel 2 70
Figure 16-1:
Instead of
a world-
line (left),
a string
creates a
worldsheet
(right) when
it moves
through
space.
One problem with both quantum field theory and string theory is that they
are constructed in a way that gets placed inside the space-time coordinate
system. General relativity, on the other hand, depicts a universe in which the
space-time is dynamic. String theorists hope string theory will solve this con-
flict between the background-dependent quantum field theory and the back-
ground-independent general relativity so that eventually dynamic space-time
will be derived out of string theory. One criticism (as discussed in Chapter 17)
is that string theory is, at present, still background-dependent.
The competing theory, loop quantum gravity, incorporates space into the
theory, but is still mounted on a background of time coordinates. Loop quan-
tum gravity is covered in more detail in Chapter 18.
HaWkinq's chronology protection
conjecture: \lou're not qoinq
anywhere
The concept of time travel is often closely tied to infinities in the curvature
of space-time, such as that within black holes. In fact, the discoveries of
mathematically possible time travel were found in the general relativity equa-
tions containing extreme space-time curvature. Stephen Hawking, one of the
most renowned experts in looking at space-time curvature, believes that time
travel is impossible and has proposed a chronology protection conjecture that
some mechanism must exist to prevent time travel.
2o(/ P art '^ : The Unseen Cosmos: String Theory On the Boundaries of Knowledge
When black holes were first proposed as solutions to Einstein's field equations,
neither Einstein nor Eddington believed they were real. In a speech to a Royal
Astronomical Society, Eddington said of black hole formation, "I think there
should be a law of nature to prevent a star from behaving in this absurd way!"
Although Hawking is certainly comfortable with the idea of black holes, he
objects to the idea of time travel. He proposed his chronology protection
conjecture, which states that there must be something in the universe that
prevents time travel.
Hawking's sometimes collaborator, Oxford physicist Roger Penrose, made
the much more guarded claim that all singularities would be protected by
an event horizon, which would shield them from direct interaction with our
normal space-time, known as the cosmic censorship conjecture. This would
also potentially prevent many forms of time travel from being accessible to
the universe at large.
One major reason time travel causes so much trouble for physics (and must
therefore be prohibited, according to Einstein and Hawking) is that you could
create a way of generating an infinite amount of energy. Say you had a portal
into the past and shone a laser into it. You set up mirrors so the light coming
out of the portal is deflected back around to go into the portal again, in
tandem with the original beam you have set up.
Now the total intensity of light coming out of the portal (in the past) would
be (or have been) twice the original laser light going in. This laser light is
sent back through the portal, yielding an output of four times as much light
as originally transmitted. This process could be continued, resulting in liter-
ally an infinite amount of energy created instantaneously.
Obviously, such a situation is just one of many examples why physicists tend
to doubt the possibility of time travel (with a few notable exceptions, which
I cover throughout this chapter). If time travel were possible, then the pre-
dictive power of physics is lost, because the initial conditions are no longer
trustworthy! The predictions based on those conditions would, therefore, be
completely meaningless.
Slortinq lime to a Standstill
With Relativity
In physics, time travel is closely linked to Einstein's theory of relativity,
which allows motion in space to actually alter the flow of time. This effect is
known as time dilation and was one of the earliest predictions of relativity.
This sort of time travel is completely allowed by the known laws of physics,
but it allows only travel into the future, not into the past.
.Chapter 16: Have Time, Will Travel 28 1
In this section I explore the special cases in relativity that imply that time
travel — or at least altered motion through time — may in fact be possible.
Skip ahead to "General Relativity and Wormholes: Doorways in Space and
Time" for more information about how the general theory of relativity relates
to potential time travel.
Time dilation and black hole event horizons, both of which I explain in the
following sections, provide intriguing ways of extending human life, and in sci-
ence fiction they've long provided the means for allowing humans to live long
enough to travel from star to star. (See the later sidebar "The science fiction of
time" for more information on this.)
Time dilation: Sometimes eVen
the best Watches run slow
The most evident case of time acting oddly in relativity, and one that has
been experimentally verified, is the concept of time dilation under special
relativity. Time dilation is the idea that as you move through space, time
itself is measured differently for the moving object than the unmoving object.
For motion that is near the speed of light, this effect is noticeable and allows
a way to travel into the future faster than we normally do.
One experiment that confirms this strange behavior is based on unstable
particles, pions and muons. Physicists know how quickly the particles would
decay if they were sitting still, but when they bombard Earth in the form of
cosmic rays, they're moving very quickly. Their decay rates don't match the
predictions, but if you apply special relativity and consider the time from the
particle's point of view, the time comes out as expected.
In fact, time dilation is confirmed by a number of experiments. In the Hafele-
Keating experiments of 1971, atomic clocks (which are very precise) were
flown on airplanes traveling in opposite directions. The time differences
shown on the clocks, as a result of their relative motion, precisely matched
the predictions from relativity. Also, global positioning system (GPS) satel-
lites have to compensate for this time dilation to function properly. So time
dilation is on very solid scientific ground.
Time dilation leads to one popular form of time travel. If you were to get into
a spaceship that traveled very quickly away from Earth, time inside the ship
would slow down in comparison to that on Earth. You could do a flyby of a
nearby star and return to Earth at nearly the speed of light, and a few years
would pass on Earth while possibly only a few weeks or months would pass
for you, depending on how fast you were going and how far away the star was.
The biggest problem with this is how to accelerate a ship up to those speeds.
Scientists and science fiction authors have made various proposals for such
282 P art '^ : The Unseen Cosmos: String Theory On the Boundaries of Knowledge
devices, but all are well outside the range of what we could feasibly build
today or in the foreseeable future.
vjjJftBEfl As you accelerate an object to high speeds, its mass also increases, which
$Tir %\ means it takes more and more energy to keep accelerating it. This formula of
( iSO ) mass increase is similar to the formula that describes time dilation, so this
\UB/ makes it fundamentally difficult to get significant levels of time dilation.
The question is how much time dilation you really need, though, especially
for trips within only a few light-years of Earth. One strange potential byprod-
uct of this form of time travel is described toward the end of this chapter in
the section entitled "The twin paradox."
Black hole event horizons: An extra-stout
Version of stow motion
One other case where time slows down, this time in general relativity, involves
black holes. Recall that a black hole bends space-time itself, to the point where
even light can't escape. This bending of space-time means that as you approach
a black hole, time will slow down for you relative to the outside world.
If you were approaching the black hole and I were far away watching (and
could somehow watch "instantly," without worrying about the time lag from
light speed), I would see you approach the black hole, slow down and eventu-
ally come to rest to hover outside of it. Through the window of your space-
ship, I would see you sitting absolutely still.
You, on the other hand, would not notice anything in particular — at least
until the intense gravity of the black hole killed you. But until then, it certainly
wouldn't "feel" like time was moving differently. You'd have no idea that as you
glide past the black hole's event horizon (which you possibly wouldn't even
notice), thousands of years were passing outside of the black hole.
As you find out in the next section, some believe that black holes may actu-
ally provide a means to more impressive forms of time travel as well.
General Relativity and Wormhotes:
Dooru/ays in Space and Time
In general relativity, the fabric of space-time can occasionally allow for world-
lines that create a closed timelike curve, which is relativity-speak for time
travel. Einstein himself explored these concepts when developing general
.Chapter 16: Have Time, Will Travel 283
relativity, but never made much progress on them. In the following years,
solutions allowing for time travel were discovered.
The first application of general relativity to time travel was by the Scottish
physicist W. J. van Stockum in 1937. Van Stockum imagined (in mathemati-
cal form, because that's how physicists imagine things) an infinitely long,
extremely dense rotating cylinder, like an endless barbershop pole. It turns
out that in this case, the dense cylinder actually drags space-time with it, cre-
ating a space-time whirlpool.
This space-time whirlpool is an example of a phenomenon called frame drag-
ging. It takes place when an object "drags" space (and time) along with it. This
frame dragging is in addition to the normal bending of space-time due to grav-
ity and is due to the movement of incredibly dense objects in space, such as
neutron stars. This is similar to how an electric mixer causes the surrounding
cake batter to swirl. This effect is frequently exploited to come up with time-
travel solutions.
In van Stockum's situation, you could fly up to the cylinder in a spaceship
and set a course around the cylinder and arrive back at a point in time before
you arrived at the cylinder. In other words, you can travel into the past along
a closed timelike curve. (If you can't picture this path, don't feel bad. The
path is in four dimensions, after all, and results in going backward in time, so
it's clearly something our brains didn't evolve to picture.)
Another theory about time travel was proposed in 1949 by Einstein's colleague
and friend at Princeton University's Institute for Advanced Study, the mathemati-
cian Kurt Godel. Godel considered the situation where all of space — the entire
universe itself — was actually rotating. You might ask if everything is rotating
how we'd ever know it. Well, it turns out that if the universe were rotating,
according to general relativity, then we'd see laser beams curve slightly as they
move through space (beyond the normal gravitational lensing, where gravity
bends light beams).
The solution that Godel arrived at was disturbing, because it allowed time
travel. It was possible to create a path in a rotating universe that ended
before it began. In Godel's rotating universe, the universe itself could func-
tion as a time machine.
So far, physicists haven't found any conclusive evidence that our universe is
rotating. In fact, the evidence points overwhelmingly toward the idea that it's
not. But even if the universe as a whole doesn't rotate, objects in it certainly do.
2oQ Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
Taking a shortcut through space and time
With a Wormhole
In a solution called an Einstein-Rosen bridge (shown in Figure 16-2 and more
commonly called a wormhole), two points in space-time could be connected
by a shortened path. In some special cases, a wormhole may actually allow
for time travel. Instead of connecting different regions of space, the worm-
hole could connect different regions of time!
Wormholes were studied by Albert Einstein and his pupil Nathan Rosen in
1935. (Ludwig Flamm had first proposed them in 1916.) In this model, the
singularity at the center of a black hole is connected to another singularity,
which results in a theoretical object called a white hole.
While the black hole draws matter into it, a white hole spits matter out.
Mathematically, a white hole is a time-reversed black hole. Because no one's
ever witnessed a white hole, it's probable that they don't exist, but they are
allowed by the equations of general relativity and haven't been completely
ruled out yet.
An object falling into a black hole could travel through the wormhole and
come out the white hole on the other side in another region of space. Einstein
showed that there were two flaws with using a wormhole for time travel:
.Chapter 16: Have Time, Will Travel 285
Iv" A wormhole is so unstable that it would collapse in upon itself almost
instantaneously.
u* Any object going into a black hole would be ripped apart by the intense
gravitational force inside the black hole and would never make it out the
other side.
Then, in 1963, New Zealand mathematician Roy Kerr calculated an exact solu-
tion for Einstein's field equations representing a Kerr black hole. The special
feature of a Kerr black hole is that it rotates. So far as scientists know, all
objects in the universe rotate, including stars, so when the star collapses into
a black hole, it's likely that it too will rotate.
In Kerr's solution, it's actually possible to travel through the rotating black
hole and miss the singularity at the center, so you could come out the other
side. The problem is, again, that the black hole would probably collapse as
you're going through it. (I address this problem in the next section.)
Assuming physicists could get a wormhole to be large and stable enough
to pass through, probably the simplest time machine that could use
this method was theorized by Kip Thorne of the California Institute of
Technology. Consider a wormhole with the following features:
(<" One end of the wormhole is on Earth.
i^ The other end of the wormhole is located inside a spaceship, currently
at rest on Earth. The end in the spaceship moves when the spaceship
moves.
v" You can travel through the wormhole either way, or talk through it, and
such travel or communication is essentially instantaneous.
Now assume that a pair of twins, named Maggie and Emily, are standing at
either end of the wormhole. Maggie is next to the wormhole on Earth in 2009,
while Emily is on the spaceship (also, for the moment, in 2009). She goes on a
little jaunt for a few days, traveling at nearly the speed of light, but when she
comes back, thousands of years have passed on Earth due to time dilation
(she is now in 5909).
On Maggie's side of the wormhole (still 2009), only a few days have passed.
In fact, the twins have regularly been discussing the strange sights that Emily
has witnessed over the few days of her journey. Emily (in 5909) is able to go
through the wormhole to Maggie's location (in 2009) and, voila, she has trav-
eled back in time thousands of years!
In fact, now that Emily's gone to the trouble of setting up the portal, Maggie
(or anyone else) could just as easily travel from 2009 to 5909 (or vice versa)
just by stepping through it.
2o0 P art '^ : The Unseen Cosmos: String Theory On the Boundaries of Knowledge _
4/ w\ Since Thome's model, there have been several wormhole-based time travel
|M|| ] scenarios developed by physicists. In fact, some physicists have shown that if
a wormhole exists, it has to allow travel in time as well as space.
Overcoming a Wormhole's instability
With negative energy
The problem with using wormholes to travel in space or time is that they are
inherently unstable. When a particle enters a wormhole, it creates fluctua-
tions that cause the structure to collapse in upon itself. There are theories
that a wormhole could be held open by some form of negative energy, which
represents a case where the energy density (energy per volume) of space is
actually negative.
Under these theories, if a sufficient quantity of negative energy could be
employed, it might continue to hold the wormhole open while objects pass
through it. This would be an absolute necessity for any of the previously
discussed theories that allow a wormhole to become a time portal, but
scientists lack a real understanding of how to get enough negative energy
together, and most think it's an impossible task.
In some models, it may be possible to relate dark energy and negative energy
(both exhibit a form of repulsive gravity, even though dark energy is a posi-
tive energy), but these models are highly contrived. The good news (if you
see possible time travel as good news) is that our universe appears to have
dark energy in abundance, although the problem is that it looks like it's
evenly distributed throughout the universe.
Trying to find any way to store negative energy and use it to sustain a worm-
hole's stability is far beyond current technology (if it's even possible at all).
String theory can provide potential sources of negative energy, but even in
these cases, there's no guarantee stable wormholes can occur.
Crossing Cosmic Strings
to AiiovO Time Travel
Cosmic strings are theoretical objects that predate string theory, but in
recent years there's been some speculation that they may actually be
enlarged strings left over from the big bang, or possibly the result of branes
colliding. There has also been speculation that they can be used to create a
time machine.
.Chapter 16: Have Time, Will Travel 28 7
Regardless of their origin, if cosmic strings exist, they should have an
immense amount of gravitational pull, and this means that they can cause
frame dragging. In 1991, J. Richard Gott (who, with William Hiscock, solved
Einstein's field equations for cosmic strings in 1985) realized that two cosmic
strings could actually allow time travel.
The way this works is that two cosmic strings cross paths with each other in
a certain way, moving at very high speeds. A spaceship traveling along the
curves could take a very precise path (several of which were worked out by
Curt Cutler in the months after Gott's publication) and arrive at its starting
position, in both space and time, allowing for travel in time. Like other time
machines, the spaceship couldn't travel further back than when the cosmic
strings originally got in position to allow the travel — in essence, the time
travel is limited to when the cosmic string time machine was activated.
Gott's was the second time machine (following Kip Thome's) to have been
published in a major journal in the early 1990s, and it sparked a wave of work
in the area. In May 1991, Gott was featured in Time magazine. In the summer
of 1992, physicists held a conference on time travel at the Aspen Center for
Physics (the same place where, nearly a decade earlier, John Schwartz and
Michael Green had determined that string theory could be consistent).
When Gott proposed this model, cosmic strings were believed to have noth-
ing to do with string theory. In recent years, physicists have grown to believe
that cosmic strings, if they exist, may actually be very closely related to
string theory.
A Tu/o~Timiny Science: String Theory
Makes More Time dimensions Possible
Because relativity showed time as one dimension of space-time and string
theory predicts extra space dimensions, a natural question would be whether
string theory also predicts (or at least allows for) extra time dimensions.
According to physicist Itzhak Bars, this may actually be the case, in a field
he calls two-time physics. Though still a marginal approach to string theory,
understanding this potential extra dimension of time could lead to amazing
insights into the nature of time.
Adding a new time dimension
With one time dimension, you have the arrow of time, but with two time
dimensions, things become less clear. Given two points along a single time
dimension, there's only one path between them. With two time dimensions,
2oO P art 'V ; The Unseen Cosmos: String Theory On the Boundaries of Knowledge
two points can potentially be connected by a number of different paths, some
of which could loop back on themselves, creating a route into the past.
Most physicists have never looked into this possibility, for the simple
fact that (in addition to making no logical sense) it wreaks havoc with the
mathematical equations. Time dimensions have a negative sign, and if you
incorporate even more of them you can end up with negative probabilities of
something happening, which is physically meaningless.
However, Itzhak Bars of the University of Southern California in Los
Angeles discovered in 1995 that M-theory allowed for the addition of an
extra dimension — as long as that extra dimension was timelike.
To get this to make any sense, he had to apply another type of gauge symme-
try, which placed a constraint on the way objects could move. As he explored
the equations, he realized that this gauge symmetry only worked if there
were two extra dimensions — one extra time dimension and one extra space
dimension. Two-time relativity has four space dimensions and two time
dimensions, for a total of six dimensions. Two-time M-theory, on the other
hand, ends up with 13 total dimensions — 11 space dimensions and two time
dimensions.
The gauge symmetry that Bars introduced provided exactly the constraint he
needed to eliminate time travel and negative probabilities from his theory.
With his gauge symmetry in place, the world with six (or 13) dimensions
should behave exactly like the world with four (or 1 1) dimensions.
Reflecting Wo-time onto
a one-time universe
In a 2006 paper, Bars showed that the Standard Model is a shadow of his
6-dimensional theory. Just like a 2-dimensional shadow of a 3-dimensional
object can vary depending on where the light source is placed, the 4-dimen-
sional physical properties ("shadows") can be caused by the behavior of the
6-dimensional objects. The objects in the extra dimensions of Bars's two-time
physics theory can have multiple shadows in the 4-dimensional universe (like
ours), each of which corresponds to different phenomena. Different physical
phenomena in our universe can result from the same fundamental 6-dimen-
sional objects, manifesting in different ways.
To see how this works, consider a particle moving through empty space in six
dimensions, with absolutely no forces affecting it. According to Bars's calcu-
lations, such activity in six dimensions relates to at least two shadows (two
physical representations of this 6-dimensional reality) in the 4-dimensional
world:
.Chapter 16: Have Time, Will Travel 28 9
U* An electron orbiting an atom
J-" A particle in an expanding universe
Bars believes that two-time physics can explain a puzzle in the Standard
Model. Some parameters describing quantum chromodynamics (QCD) have
been measured to be quite small, meaning that certain types of interactions
are favored over others, but nobody knows why this is. Physicists have come
up with a possible fix for this, but it involves predicting a new theoretical par-
ticle called an axion, which has never been observed.
According to Bars's predictions, two-time physics presents a 4-dimensional
world in which QCD interactions are not at all lopsided, so the axion isn't
needed. Unfortunately, the lack of discovery of an axion isn't really enough to
be counted as experimental proof of two-time physics.
For that, Bars has applied two-time physics to supersymmetry. In this case,
the superpartners predicted have slightly different properties than the super-
partners predicted by other theories. If superpartners are observed at the
Large Hadron Collider with the properties Bars suggests, this would be con-
sidered intriguing experimental evidence in favor of his claims.
Does Wo-time physics ha</e
any real applications)
Most physicists believe that these extra-dimensional results from Bars are
just mathematical artifacts. Several theorists, including Stephen Hawking,
have used the idea of imaginary time dimensions (an imaginary quantity
in mathematics is the square root of a negative number), but rarely is this
believed to have a real physical existence. To most physicists, they're math-
ematical tools that simplify the equations.
However, history has shown that "mathematical artifacts" can frequently
have a real existence. Bars himself seems to believe that they have as much
physical reality as the four dimensions that we know exist, although we'll
never experience these extra dimensions as directly.
Though two-time physics doesn't directly imply any time travel, if it's true, it
means that time is inherently more complex than physicists have previously
believed. Unraveling the mystery of two-time physics could well introduce
new ways that time travel might manifest in our universe.
2y(/ P ar t 'V: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
Sending Messages through Time
The original string theory, bosonic string theory, contained a massless
particle called the tachyon, which travels faster than the speed of light. In
Chapter 10, 1 explain how these particles are usually a sign that a theory has
an inherent flaw — but what if they actually existed? Would they allow a
means of time travel?
The short answer is that no one knows. The presence of tachyons in a theory
means that things begin to go haywire, which is why they're considered
by physicists to be a sign of fundamental instabilities in the theory. (These
instabilities in string theory were fixed by including supersymmetry, creating
superstring theory — see Chapter 10.)
However, just because tachyons mess up the mathematics that physicists
use doesn't necessarily mean that they don't exist. It may be possible that
physicists just haven't developed the proper mathematical tools to address
them in a way that makes sense.
If tachyons do exist, then in theory it would be possible to send messages
that travel faster than the speed of light. These particles could actually travel
backward in time and, in principle, be detected.
To avoid this problem (because, remember, time travel can destroy all of
physics!), the physicist Gerald Feinberg presented the Feinberg reinterpreta-
tion principle in 1967, which says that a tachyon traveling back in time can
be reinterpreted, under quantum field theory, as a tachyon moving forward
in time. In other words, detecting tachyons is the same as emitting tachyons.
There's just no way to tell the difference, which would make sending and
receiving messages fairly challenging.
Time Trai/el Paradoxes
Time travel inherently creates a number of logical inconsistencies, called
paradoxes. These problems have created some of the finest science fiction
tales and films (see the nearby sidebar), and have troubled philosophers and
scientists since they were first posed. Whether these inconsistencies mean
that time travel is physically impossible remains to be seen, although they're
among the reasons why most physicists tend to believe that time travel is
impossible.
.Chapter 16: Have Time, Will Travel %ty /
The Win paradox
The twin paradox is one of the classic examples of Einstein's theory of relativ-
ity in action and dates back nearly as far as the theory itself. It is a thought
experiment that exhibits the strange results of time dilation. (Technically, the
twin paradox isn't a paradox so much as a problem of inconsistent measure-
ments, but the name has stuck.)
Imagine our pair of twins, Maggie and Emily, once again. At age 20, Emily
chooses to become an astronaut, getting recruited onto the first interstellar
mission. Her ship is heading to a star that is 10 light-years away, but the ship
will be traveling at nearly the speed of light, so time dilation will be in effect.
The ship is truly a wonder, and thanks to time dilation, the entire trip takes
only a couple of months from Emily's standpoint. She explores the distant
region for eight months, collecting much fascinating data. She then returns,
which also takes a couple of months. The entire trip takes Emily one year.
Maggie, on the other hand, stays on Earth. Because Emily was traveling to a
star 10 light-years away at nearly the speed of light, Emily arrives at the star
when Maggie is about 30 years old. She starts her return trip eight months
later, and that leg of the trip also takes 10 years.
The twins have a tearful reunion, where the twin paradox suddenly becomes
clear to each of them as the 41-year-old Maggie embraces her twin sister
Emily, who appears to be 21 years old. Here is the "paradox:"
What is Emily's actual age?
After all, Emily was born 41 years ago, the same time Maggie was. There is a
logical sense in which Emily is 41 years old. On the other hand, by her "bio-
logical clock" only 21 years have passed, and she certainly doesn't look 41.
There isn't a single solution to the twin paradox, because the flow of time
depends on how you choose to measure it. Time is, if you'll excuse the
phrase, relative.
No doubt if space travel ever becomes feasible, conventions of measuring
time will need to be made. For example, if the legal drinking age is 21, can an
18-year-old who has spent four years traveling at near lightspeed buy alcohol
legally?
<£ y <d P art 'V: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
The grandfather paradox
Another paradox is called the grandfather paradox and comes up in cases
where you can time travel into the past. If you travel into the past, it should
be possible to alter the past. The grandfather paradox asks:
What happens if you change the past in a way that results in you being
unable to go into the past in the first place?
Consider the classic example (which gives the paradox its name):
1. You travel into the past and accidentally cause the death of your own
grandfather.
2. You cease to exist, and therefore do not travel into the past.
3. You do not cause the death of your grandfather.
4. You now exist, so continue back to step 1.
There are two logical resolutions to the paradox. (See the sidebar "The sci-
ence fiction of time" for examples of both of these resolutions, in the form of
Back to the Future and Somewhere in Time.)
The first is based off of the many world interpretation (MWI) of quantum
physics. In this view, many possible timelines exist and we exist in one of
them. If you travel back in time and alter time, then you will continue forward
in a different timeline than the one you initially began in.
The second possible resolution to the grandfather paradox is that it's actu-
ally impossible to alter the past. The past is set in stone, and if you travel to
the past, you'll find that you're unable to change the events that took place,
no matter how hard you try.
Unfortunately, the second possibility creates some philosophical problems
with free will, because if you are already part of the past, then that means
that your own future is set — you will definitely travel into the past at some
point. The past and the future both become set in stone.
Of course, no one knows which resolution is correct, and if Stephen
Hawking's chronology protection conjecture is true, it's very likely that the
situation never will arise. Still, it's fun to speculate on.
Where are the time travelers!
One of the most practical paradoxes brought up regarding time travel is the cur-
rent lack of any time travelers. If time travel into the past were possible, then it
would seem like people from the future would be showing up in our present.
.Chapter 16: Have Time, Will Travel 293
The science fiction of time
Talking about time travel without mentioning
science fiction would leave an elephant in the
chapter, so to speak. Here are some key sci-
ence fiction novels and films related to the
time travel concepts discussed in this chap-
ter, although the list is by no means complete.
Spoiler alert: Some plot details are revealed in
the descriptions below.
Novels:
w The Time Machine, by H. G. Wells (1895):
The first story with a man-made device to
travel in time, where the travel was under
the control of the traveler (as opposed to
stories that preceded it like Rip van Winkle,
A Connecticut Yankee in King Arthur's
Court, or A Christmas Carol, where the time
traveler had no control).
v* Tau Zero, by Poul Anderson (1967): A
spaceship is trapped accelerating closer
and closer to the speed of light, unable to
decelerate. The novel explores the effects
of time dilation and the possible end of the
universe.
v* Gateway, by Frederick Pohl (1977): The sole
survivor of a space accident has to come
to terms with intense survivor's guiltforthe
crew he left behind. The plot's powerful
climax (which I may now be ruining by tell-
ing you) relates to the idea that as you fall
into a black hole, time slows down.
Films:
i^ Somewhere in 7V/ne(1980): Richard Collier
(Christopher Reeve) is a playwright who
travels to 1912 from 1980. The film takes
the stance that the past has already hap-
pened and Collier was already part of the
events of the past (or he's hallucinating, in
which case this film has nothing to do with
time travel and is far less interesting). For
example, "before" he ever time travels, he
finds his own signature in a hotel guestbook
from 1912. Based on a novel by Richard
Matheson.
e* Back to the Future (1985): Marty McFly
(Michael J. Fox) travels from 1985 to 1955
and interferes with his parents' first meet-
ing. The film explores the concept of time
paradoxes and potential multiple timelines.
There were two sequels, but the original
film was by far the best.
i«* Frequency(200Q): New York detective John
Sullivan (James Caviezel) begins commu-
nicating with his father (Dennis Quaid) 30
years in the past over a ham radio, which
is bouncing signals off of strange sunspot
activity. In this film, no material objects
travel in time — only information in the form
of radio waves. String theorist and author
Brian Greene served as physics consultant
and had a cameo in the film.
Not only do science fiction authors learn from
scientists in developing their time travel sys-
tems, but inspiration can flow the other way.
Dr. Ronald Mallet, who is trying to build a
time machine, was motivated throughout his
life by science fiction accounts of time travel.
Kip Thorne has developed his theories of time
travel out of helping friends work out the details
of their science fiction novels. His first work on
time travel was based on work performed to
help Carl Sagan develop a realistic wormhole
for his novel Contact in the 1980s, and he later
gained insights from the science fiction author
Robert Forward.
<£yll Part IV: The Unseen Cosmos: String Theory On the Boundaries of Knowledge
The solution to this question in the Star Trek universe is the "temporal prime
directive," which basically makes the argument that time travelers are for-
bidden from interfering in the past. In this way, any time travelers among us
would have to stay hidden.
A more scientific solution is the idea that time travel is only allowed after a
time travel device has been constructed. When the device is active, you could
use it to travel in time, but you obviously could never go to a time period
before the device was created. In fact, every time machine that scientists have
found that could exist in our universe has this very feature — you can never go
back to before the invention (and activation) of the time machine.
PartV
What the Other Guys Say:
Criticisms and
Alternatives
The 5 th Wave
By Rich Tennant
-rv ma wm nr— ri ar~" i~ < << in u\
"I just can't help "believing that siring theory is
our "best weans o£ understanding this cra7.y
universe v*e live in.*
In this part .
J\ lot everyone embraces string theory as the theory
W W that will answer the fundamental questions of
physics. In fact, in recent years, even some string
theorists have begun backing off of that claim.
In this part, I explain some of the major criticisms of
string theory in recent years. I then explore the major
alternative quantum gravity theory, loop quantum gravity,
and other directions of research that may provide
insights, regardless of whether string theory ultimately
fails or succeeds. If string theory does fail, or even if it
succeeds but not as a "theory of everything," these
alternative approaches may prove useful in filling the
gaps. Some of these research efforts may provide clues
that could help with the progress of string theory.
Chapter 17
Taking a Closer Look at the String
Theory Controversy
In This Chapter
Considering what string theory does and doesn't explain
Realizing that string theory may never explain our universe
Should string theorists control physics departments and research funding?
A\ lthough many physicists believe that string theory holds the promise
¥ \ as the most likely theory of quantum gravity, there's a growing skepticism
among some that string theory hasn't achieved the goals it set out for. The
major thrust of the criticism is that, whatever useful benefits there are to
studying string theory, it's not actually a fundamental theory of reality, but
only a useful approximation.
String theorists acknowledge some of these criticisms as valid and dismiss
others as premature or even completely contrived. Whether or not the
critics are right, they've been a part of string theory since the very first days
and are likely to be around as long as the theory persists. Lately, the criticism
has risen to such furor that it's being called "the string wars" across many
science blogs and magazines.
In this chapter, I discuss some of the major criticisms of string theory. I begin
with a brief recap of the history of string theory, from the eye of the skeptic,
who focuses on the failures instead of the successes. After that, I look into
whether string theory has any ability to actually provide any solid predictions
about the universe. Next, you see how string theory critics object to the
extreme amount of control that string theorists hold over academic institutions
and research plans. I then consider whether string theory possibly describes
our own reality. And, finally, I explain some of the major string theory
responses to these criticisms.
2y8 Part V: Wnat tne 0tner Gu V s Sa V : Criticisms and Alternatives
The String Wars: Outlining
the Arguments
As long as it's been around, string theory has contended with criticisms.
Some of string theory's critics are among the most respected members of
the physics community, including Nobel laureates such as Sheldon Glashow
and the late Richard Feynman, both of whom were critical as far back as the
first superstring revolution in the mid-1980s. Still, string theory has steadily
grown in popularity for decades.
Recently, the rise in criticisms against string theory has spilled into the
popular media, making the front pages of science magazines and even large
articles in more mainstream publications. The debate rages across radio
waves, the Internet, academic conferences, the blogosphere, and anywhere
else that debates are allowed to rage.
Though the debate sounds passionate, none of the critics are really
advocating that physicists completely abandon string theory. Instead, they
tend to view string theory as an effective theory (a useful approximation)
rather than a truly fundamental theory, which describes the most basic level
of reality itself. They are critical of string theorists' attempts to continue to
promote the theory as a fundamental theory of reality.
Here are some of the most significant criticisms levied against string theory
(or the string theorists who practice it):
v* String theory is unable to make any useful prediction about how the
physical world behaves, so it can't be falsified or verified.
v* String theory is so vaguely defined and lacking in basic physical
principles that any idea can be incorporated into it.
J-" String theorists put too much weight on the opinions of leaders and
authorities within their own ranks, as opposed to seeking experimental
verification.
u* String theorists present their work in ways that falsely demonstrate
that they've achieved more success than they actually have. (This isn't
necessarily an accusation of lying, but may be a fundamental flaw in how
success is measured by string theorists and the scientific community at
large.)
i^ String theory gets more funding and academic support than other
theoretical approaches (in large part because of the aforementioned
reported progress).
u* String theory doesn't describe our universe, but contradicts known facts
of physical reality in a number of ways, requiring elaborate hypothetical
constructions that have never been successfully demonstrated.
Chapter 17: Taking a Closer Look at the String Theory Controversy £yy
Behind many of these criticisms is the assumption that string theory, which
has been around for 30 years, should be a bit more fully developed than it
actually is. None of the critics are arguing to abandon the study of string
theory; they just want alternative theories to be pursued with greater
intensity, because of the belief that string theory is falling short of the mark.
To explore the validity of these claims and determine whether string theory
is in fact unraveling, it's necessary to lay out the frame of the debate by
looking at where string theory has been and where it is today.
Thirty years and counting: Framing the
debate from the skeptic's point of View
Even now, with criticism on the rise, it doesn't appear that the study of string
theory has dropped. To understand why physicists continue to study string
theory, and why other physicists believe it isn't delivering as promised, let
me briefly recount the general trends in the history of string theory, focusing
this time on its shortcomings. (This material is presented in significantly
greater detail in Chapters 10 and 11.)
String theory started in 1968 as a theory (called the dual resonance model) to
predict the interactions of hadrons (protons and neutrons), but failed at that.
Instead of this model, quantum chromodynamics, which said that hadrons were
composed of quarks held together by gluons, proved to be the correct model.
Analysis of the early version of string theory showed that it could be viewed
as very tiny strings vibrating. In fact, this bosonic string theory had several
flaws: fermions couldn't exist and the theory contained 25 space dimensions,
tachyons, and too many massless particles.
These problems were "fixed" with the addition of supersymmetry, which
transformed bosonic string theory into superstring theory. Superstring
theory still contained nine space dimensions, though, so most physicists still
believed it had no physical reality.
This new version of string theory was shown to contain a massless, spin-2
particle that could be the graviton. Now, instead of a theory of hadron
interactions, string theory was a theory of quantum gravity. But most
physicists were exploring other theories of quantum gravity, and string
theory languished throughout the 1970s.
The first superstring revolution took place in the mid-1980s, when physicists
showed ways to construct string theory that made all the anomalies go away.
In other words, string theory was shown to be consistent. In addition, physicists
found ways to compactify the extra six space dimensions by curling them up
into complex shapes that were so tiny they would never be observed.
300 Part V: Wnat tne 0ther Guvs Sa V : Criticisms and Alternatives _
The rise in work on string theory had great results. In fact, the results were
too good, because physicists discovered five distinct variations of string
theory, each of which predicted different phenomena in the universe and
none of which precisely matched our own.
In 1995, Edward Witten proposed that the five versions of string theory were
different low-energy approximations of a single theory, called M-theory.
This new theory contained ten space dimensions and strange objects called
branes, which had more dimensions than strings.
A major success of string theory was that it was used to construct a
description for black holes, which calculated the entropy correctly, according
to the Hawking-Bekenstein predictions for black hole thermodynamics. This
description applied only to specific types of simplified black holes, although
there was some indication that the work might extend to more general black
holes.
A problem for string theory arose in 1998, when astrophysicists showed that
the universe was expanding. In other words, the cosmological constant of
the universe is positive, but all work in string theory had assumed a negative
cosmological constant. (The positive cosmological constant is commonly
referred to as dark energy.)
In 2003, a method was found to construct string theory in a universe that had
dark energy, but there was a major problem with it: A vast number of distinct
string theories were possible. Some estimates have been as much as 10 500
distinct ways to formulate the theory, which is so absurdly large that it can
be treated as if it were basically infinity.
As a response to these findings, physicist Leonard Susskind proposed the
application of the anthropic principle as a means of explaining why our
universe had the properties it did, given the incredibly large number of
possible configurations, which Susskind called the landscape.
This brings us to the current status of string theory, in very broad strokes.
You can probably see some chinks in string theory's armor, where the
criticisms seem to resonate particularly strongly.
A rise of criticisms
After evidence of dark energy was discovered in 1998 and the 2003 work
increased the number of known solutions, there seemed to be some growth
in criticisms. The attempts to make the theory fit physical reality were
growing a bit more strained, in the eyes of some, and a discontent that had
always existed under the surface began to seep out of the back rooms at
physics conferences and onto the front pages of major science magazines.
Chapter 17: Taking a Closer Look at the String Theory Controversy 3v /
While innovative new variants — such as the Randall-Sundrum models and
the incorporation of a positive cosmological constant — were rightly
recognized as brilliant, some people believed that physicists had to come
up with contrived explanations to keep the theory viable.
The growth in criticism became glaringly obvious to the general public in
2006 with the publication of two books criticizing — or outright attacking —
string theory. The books were Lee Smolin's The Trouble with Physics: The
Rise of String Theory, the Fall of a Science, and What Comes Next and Peter
Woit's Not Even Wrong: The Failure of String Theory and the Search for Unity in
Physical Law. These books, along with the media fervor that accompanies
any potential clash of ideas, has put string theory on the public relations
defensive even while many (possibly most) string theorists dismiss the
Smolin and Woit claims as failed attempts to discredit string theory for their
own aggrandizement.
The truth is likely somewhere in between. The criticisms have a bit more
merit than string theorists would give them, but are not quite as destructive
as Woit, at least, would tend to have readers believe. (Smolin is a bit more
sympathetic toward string theory, despite his book's subtitle.) None of the
critics propose abandoning string theory entirely; they merely would like to
see more scientists pursuing other areas of inquiry, such as those described
in Chapters 18 and 19.
7s String Theory Scientific)
The first two criticisms cut to the core of whether string theory is successful
as a scientific theory. Not just any idea, not even one that's expressed in
mathematical terms, is scientific. In the past, to be scientific, a theory had to
describe something that is happening in our own universe. To go too far from
this boundary enters the realm of speculation. Criticisms of string theory as
unscientific tend to fall in two (seemingly contradictory) categories:
(-" String theory explains nothing.
u* String theory explains too much.
Argument No. 1: String theory
explains nothing
The first attack on string theory is that, after about 30 years of investigation,
it still makes no clear predictions. (Physicists would say it has no predictive
power.} The theory makes no unique prediction that, if true, supports the
theory and, if false, refutes the theory.
j(/2 Part V: Wnat the O ther Guys Say: Criticisms and Alternatives _
According to philosopher Sir Karl Popper, the trait of "falsifiability" is the
defining trait of science. If a theory is not falsifiable — if there is no way to
make a prediction that gets a false result — then the theory is not scientific.
^$&BE# If you subscribe to Popper's view (and many scientists don't), then string
/'^ _ ^ s \ theory is certainly not scientific — at least not yet. The question is whether
iMJj J string theory is fundamentally unable to make a clear, falsifiable prediction or
whether it merely hasn't done so yet, but will at some point in the future.
It's possible that string theorists will make a distinct prediction at some
point. Part of the criticism, though, is that string theorists are really not
concerned with making a prediction. Some string theorists don't even seem
to consider the lack of a currently testable prediction to be a shortcoming, so
long as string theory remains consistent with the known evidence.
This is what motivates the major critics of string theory, from Feynman in
the 1980s to Smolin and Woit today, to complain that string theory has no
contact with experiment and is fundamentally warping what it means to
investigate something scientifically.
Argument No. 2: String theory
explains too much
The second attack is based on the same problem, that string theory makes
no unique prediction, but the emphasis this time is on the word "unique."
There are so many variations of string theory that even if it could be
formulated in a way that it would make a prediction, it seems as if each
version of string theory would make a slightly different prediction.
This is, in a way, almost worse than making no prediction at all. With no
prediction, you can make the argument that more work and refinement needs
to be done, new mathematical tools developed, and so on. With a nearly
infinite number of predictions, you're stuck with a theory that's completely
useless. Again, it has no predictive power, for the simple reason that you can
never sort out the sheer volume of results.
Part of this argument relates back to the principle of Occam's razor.
According to this principle, there is an economy in nature, which means that
nature (as described by science) doesn't include things that aren't necessary.
String theory includes extra dimensions, new types of particles, and possibly
whole extra universes that have never been observed (and possibly can
never be observed).
Chapter 17: Taking a Closer Look at the String Theory Controversy jVj
Neiti rules to the game: The anthropic principle revisited
The solution for so many predictions, as proposed by physicist Leonard
Susskind, is to apply the anthropic principle to focus on the regions of the
string theory landscape that allow life to exist. According to Susskind, Earth
clearly exists in a universe (or a region of the universe, at least) that allows
life to exist, so selecting only theories that allow life to exist seems to be a
reasonable strategy.
Taking a theory that doesn't allow life to exist and considering it on equal
footing with theories that do allow life to exist, when we know that life does
exist, defies both scientific reasoning and common sense.
From this stance, the anthropic principle is a way of removing selection bias
when looking at different possible string theories. Instead of looking only at
the mathematical viability of a theory, as if that were the only criteria,
physicists can also select based on the fact that we live here.
However, there's a bit of clever maneuvering within this discussion that
shouldn't go unmentioned. It's not just that Susskind has said that we can use
the anthropic principle to select which theories are viable in our universe,
but he's gone further to indicate that the very fact that all of these versions
of string theory exist is a good thing. It provides a richness to the theory,
making it more robust. (Still others point out that all quantum field theories
have lots of potential solutions, so string theory shouldn't be any different.
In those cases, both sides of this particular debate are looking at it the
wrong way.)
For nearly two decades, many physicists were trying to find a single version
of string theory that included basic physical principles that dictated the
nature of the universe. The current Standard Model has 18 fundamental
particles, which have to be measured in experiment and placed into the
theory by hand. Part of the goal of string theory was to find a theory that,
based on pure physical principles and mathematical elegance, would yield a
single theory describing all of reality.
Instead, string theorists have found a virtually infinite number of different
theories (or, to be more precise, different string theory solutions) and have
apparently discovered that no fundamental law describes the universe based
on basic physical principles. Selection of the correct parameters for the
theory is, once again, left to experiment.
But instead of interpreting this as a failure and indicating that we have no
choice but to apply the anthropic principle to provide limitations on which
options are available to us, Susskind takes lemons and turns them into
lemonade by reframing the entire context of success. Success is no longer
finding a single theory, but exploring as much of the landscape as possible.
301) Part V: What the Other Guys Say: Criticisms and Alternatives _
In their book Aristotle and an Aardvark go to Washington: Understanding
Political Doublespeak Through Philosophy and Jokes, authors Thomas Cathcart
and Daniel Klein refer to this sort of technique as the "Texas sharpshooter
fallacy." Imagine the Texas sharpshooter who pulls out his pistol and fires at
the wall and then walks up and draws the bull's-eye around the location where
the shots landed.
In a (very critical) sense, this is what Susskind has done, by changing the
actual definition of success in string theory. He has (according to some)
redefined the goal of the enterprise and done so in such a way that the
current work is exactly in line with the new goal. If this new approach is valid,
yielding a way to correctly describe nature, it's brilliant. If not valid, then it's
not brilliant. (For the more favorable interpretation of the anthropic principle,
see Chapters 11 and 14.)
A similar moving target can be seen in the discussion of proton decay.
Originally, experiments to prove grand unified theories (GUTs) anticipated
that these experiments would detect the decay of a few protons every year.
No proton decays have been found, however, which has caused theorists
to revise their calculations to arrive at a lower decay rate. Except most
physicists believe that these attempts are not valid and that these GUT
approaches have been disproved. This after-the-fact change in what they're
looking for is not a valid approach to science — unless the decays are
discovered at the new rate, of course (at which point the theoretical
modification becomes a brilliant insight).
None of this is to imply that Susskind is being dishonest or manipulative in
presenting the anthropic principle as an option that he believes in. He has
very genuinely been led to this belief because of the growing number of
mathematically viable string theory solutions, which leave him with no
choice (except for abandoning string theory, which I get to in a bit).
After you accept that string theory dictates a large number of possible
solutions, and you realize that modern theories of eternal inflation dictate
that many of these solutions may well be realized in some reality, there's
very little choice, in Susskind's view, other than to accept the anthropic
principle. And there's every indication that he went through some serious
soul searching before deciding to preach the anthropic message.
Interpreting the string theory landscape
No longer is string theory looking for a single theory, but it's now trying to
pare down the vast options in the landscape to find the one, or the handful,
that may be consistent with our universe. The anthropic principle can be
used as one of the major selection criteria to distinguish theories that clearly
don't apply to our universe.
Chapter 17: Taking a Closer Look at the String Theory Controversy j(/^
The question that remains is whether string theorists (or any physicist)
should be happy about this situation.
Certainly, some are not. David Gross is not. Edward Witten seems at best
lukewarm about the prospect. Susskind and Joe Polchinski, however, seem
to have had a full conversion. They have not only resigned themselves to
accepting the circumstances, but have embraced it, despite the fact that a
few years ago both were opposed to any application of the anthropic
principle in science.
The anthropic principle seems unavoidable if there exists a vast multiverse,
where many different regions of the string theory landscape are realized in
the form of parallel universes. Some universes will exist where life is allowed,
and we're one of them — get used to it.
Some string theorists who haven't accepted the anthropic arguments are
hopeful that the theory's mathematical and physical features can rule out
large portions of the landscape. String theorists are still divided over exactly
what conclusions the theory allows and whether there might be some way to
sort them out without applying the anthropic principle. More work must be
done before anyone knows for sure.
Turning a Critical Eye to String Theorists
One of the major criticisms of string theory has to do not with the theory so
much as with theorists. The argument is that they are forming something of a
"cult" of string theorists, who have bonded together to promote string theory
above all alternatives.
This criticism, which is at the heart of Smolin's The Trouble with Physics, is
not so much a criticism of string theory as a fundamental criticism of the way
academic resources are allocated. One criticism of Smolin's book has been
that he is in part demanding more funding for the research projects that he
and his friends are working on, which he feels are undersupported. (Many of
these alternative fields are covered in Chapters 18 and 19.)
Hundreds of physicists just can't be Wrong
String theory is the most popular approach to a theory of quantum gravity,
but that very phrase — most popular — is exactly the problem in the eyes of
some. In physics, who cares (or who should care) how popular a theory is?
300 Part V: Wnat tne 0ther Gu V s Sa V : Criticisms and Alternatives _
In fact, some critics believe that string theory is little more than a cult of
personality. The practitioners of this arcane art have long ago foregone the
regular practice of science, and now bask in the glory of seer-like authority
figures like Edward Witten, Leonard Susskind, and Joe Polchinski, whose
words can no more be wrong than the sun can stop shining.
This is, of course, an exaggeration of the criticism, but in some cases, not by
much. String theorists have spent more than two decades building a community
of physicists who firmly believe that they are performing the most important
science on the planet, even while achieving not a single bit of evidence to
definitively support their version of science as the right one, and the folks at
the top of that community carry a lot of weight. (For a look at this behavior in
nonphysics contexts, see the nearby sidebar "Appeal to authority.")
John Moffat has joined Smolin and Woit in lamenting the "lost generation" of
brilliant physicists who have spent their time on string theory, to no avail.
He points out that the sheer volume of physicists publishing papers on string
theory, and in turn citing other string theorists, skews the indexes about
which papers and scientists are truly the most important.
For example, there is a rumor that Edward Witten has the highest h-index of
any living scientist. (The h-index is a measure of how often papers are cited.)
If you look at it from Moffat's point of view, this is not necessarily a result
of Witten being the most important physicist of his generation, but rather a
result of Witten writing papers that are fundamental to string theory, and, in
turn, are cited by the vast majority of people writing papers on string theory,
which is a lot of papers.
Now the problem with this approach when it comes to Witten specifically is
that it's very possible that he is the most important physicist of his generation.
Certainly his Fields Medal attests to his position as one of the most
mathematically gifted. But if he is an important physicist who has helped
lead a generation of physicists down a road that ends in string theory as a
failed theory of quantum gravity, then that would indeed make for a "lost
generation" and a tragic waste of Witten's brilliance.
Holding the keys to the academic kingdom
The theoretical physics and particle physics communities in many of the
major physics departments, especially in the United States, lean heav-
ily toward string theory as the preferred approach to a quantum gravity
theory. In fact, the growing need for diverse approaches (such as those from
Chapters 18 and 19) is maintained even by some string theorists, who realize
the importance of including conflicting viewpoints.
_ Chapter 17: Taking a Closer Look at the String Theory Controversy j(//
Appeal to authority
Although it may seem odd to many people that
scientists could be swayed byfigures of authority,
this is a fundamental part of human nature. The
"appeal to authority" was cited by Aristotle,
the father of rhetoric (the science of debate).
It has been given the Latin name argumentum
adverecundiam, and evidence from psychology
has born out that it works. People are inclined
to believe an authority figure, sometimes even
over common sense.
Marketers know thatone of the most persuasive
ways to sell something is to get a testimonial.
This is why speakers are introduced by someone
else, for example. If another person gets up and
lists the speaker's accomplishments, it means
a lot more to the listeners than if the speaker
stands up, introduces herself, and lists off her
own accomplishments. This is the case even
when the introducer knows nothing about the
person except what he reads off of a card or
teleprompter.
Whenthe person who is providing thetestimonial
is perceived as an authority figure, it's even
more potent. This is why some books have
quotes from authorities on them and why
politicians seek celebrity endorsements. I'm
sure some people voted for Barack Obama
in 2008 because Oprah Winfrey, an authority
figure if ever there was one, endorsed him
publicly.
In the case of string theory, of course, the
authority figures aren't just popular, they
are experts in physics, and string theory in
particular, so listening to their opinion on string
theory is a bit more reasonable than listening
to a single popular actor, musician, athlete, or
clergyman on whom to vote into the presidency.
Ultimately, in science (as in the rest of life)
people should use their own logic to evaluate
the arguments put forward by the experts.
Fortunately, scientists are trained to use their
logic more intently than most of society.
In a debate between Brian Greene and Lee Smolin on National Public Radio,
Greene acknowledged the need to work on areas other than string theory,
pointing out that some of his own graduate students are working on other
approaches to solving problems of quantum gravity.
Lisa Randall — whose own work has often been influenced by string theory —
describes how, during the first superstring revolution, Harvard physicists
remained more closely tied to the particle physics tradition, and to
experimental results, while Princeton researchers devoted themselves
largely to the purely theoretical enterprise of string theory. In the end, every
particle theorist at Princeton worked on string theory, which she identifies as
a mistake — and one that continues to this day.
These stances indicate that if a "string theory cult" does exist, then Brian
Greene and Lisa Randall have apparently not been inducted into it. Still, the
fact is that theoretical physics departments at several major universities
are now dominated by string theory supporters, and some feel that other
approaches are inherently marginalized by that.
3 08 Part V: Wnat tne 0ther Gu V s Sa V : Criticisms and Alternatives _
This criticism is one of the fairest, I think, because science, like any other
field of endeavor, needs criticism. Psychologists have shown that the
phenomenon of "groupthink" takes hold in situations where the only people
who are allowed a seat at the table are those who think alike. If you want to
have a robust intellectual exchange — something that's at the heart of
physics and other sciences — it's important that you include people who
will challenge your viewpoints and not just agree with them.
Some criticisms of Smolin's book have indicated that he wants some sort of
handout for himself and his buddies who aren't able to cut it in the normal grant
application process. (In the other direction, Smolin and Woit have implied that
similar economic interests are at the heart of the support for string theory.)
But if the institutes that determine how funding is allocated are dominated
by people who believe that string theory is the only viable theory, then
these alternate approaches won't get funded. Add to that the citation issues
described earlier in this chapter, which possibly make string theory look
more successful than it actually is, and there's room for valid criticism of
how funding is allocated in physics.
Still, hope for these alternatives isn't lost. As popular as string theory is, 1
believe it's likely that most theoretical physicists want to find answers more
than they want to be proved right. Physicists will gravitate (so to speak)
toward the theories that provide them the best opportunity to discover a
fundamental truth about the universe.
So long as these non-string theorists continue doing solid work in these
other areas, then they have the hope of drawing recruits from the younger
generation. Eventually, if string theorists don't find some way to make string
theory succeed, it will lose its dominant position.
Does String Theory Describe
Our Universe?
Now comes the real science question related to string theory: Does it
describe our universe? The short answer is that no, it does not. It can be
written in such a way to describe some idealized worlds that bear similarities
to our world, but it can't yet describe our world.
Unfortunately, you have to know a lot about string theory to realize that.
String theorists are rarely upfront about how far their theory is from
describing our reality (when talking to public audiences, at least). It tends
to be a disclaimer, woven into the details of their presentations or thrown
in just near the end. In fact, you could read many of the books out there on
string theory and, after turning the last page, you wouldn't have ever been
told explicitly that it doesn't describe our universe.
_ Chapter 17: Taking a Closer Look at the String Theory Controversy J(/y
Congratulations on not choosing one of those books.
Making sense of extra dimensions
The world described by string theory has at least 6 more space dimensions
than the 3 we know, for a total of 9 space dimensions. In M-theory, there
are at least 10 space dimensions, and in the two-time M-theory, there are 11
space dimensions (with 2 time dimensions tacked on).
The problem is that physicists don't know where these extra dimensions are.
In fact, the main reason for believing that they exist is that the equations of
string theory demand them. These extra dimensions have been compactified
(in some models) in ways that their particular geometry generates certain
features of our universe.
There are two major ways of dealing with the extra dimensions:
j-" The extra dimensions are compactified, probably at about the Planck
scale (although some models allow for them to be larger).
j-" Our universe is "stuck" on a three space dimensional brane (brane
world scenarios).
There is another alternative: The extra dimensions may not exist. (This
would be the approach suggested by applying Occam's razor.) Various
physicists have developed approaches to string theory without extra
dimensions, as discussed in Chapter 13, so abandoning the idea of
extra dimensions doesn't even require an abandonment of string theory!
Space-time should be fluid
One of the hallmarks of modern physics is general relativity. The clash
between general relativity and quantum physics is part of the motivation
for looking for a string theory, but some critics believe that string theory is
designed in such a way that it doesn't faithfully maintain the principles of
general relativity.
Which principles of general relativity aren't maintained in string theory?
Specifically, the idea that space-time is a dynamic entity that responds to
the presence of matter around it. In other words, space-time is flexible. In
physics terminology, general relativity is a background-independent theory,
because the background (space-time) is incorporated into the theory. A
background-dependent theory is one where objects in the theory are sort of
"plugged in" to a space-time framework.
3 # v Part V: What the Other Guys Say: Criticisms and Alternatives _
Right now, string theory is a background-dependent framework. Space-time is
rigid, instead of flexible. If you are given a certain configuration of space-time,
you can discuss how a given version of string theory would behave in that
system.
The question is whether string theory, which right now can only be formulated
in fixed space-time environments, can really accommodate a fundamentally
dynamic space-time framework. How can you turn the rigid space-time of
string theory into the flexible space-time of general relativity? The pessimist
replies "You can't" and works on loop quantum gravity (see Chapter 18).
The optimist, however, believes that string theory still has hope. Even with
a rigid background of space-time, it's possible to get general relativity as a
limiting case of string theory. This isn't quite as good as getting a flexible
space-time, but it means that string theory certainly doesn't exclude general
relativity. Instead of getting the full high-definition version of space-time,
though, you're left with something more like a flipbook, which treats each
image as static but, overall, provides the impression of smooth motion.
String theory is a work-in-progress, and it's still hoped that physical and
mathematical principles might be developed that will allow for the
expression of a fully dynamic background in string theory. String theorists
are forced to talk about the theory in a rigid space-time (background
dependent) only because they haven't yet found a mathematical language
that will let them talk about it in a flexible space-time (background-independent).
Some believe that Maldacena's AdS/CFT correspondence may provide a
means of incorporating this background-independent language. It's also
possible that the principles that allow this new language will come from an
unexpected direction, such as the work described in Chapters 18 and 19.
Or, of course, such principles may not exist at all, and the skeptic's
inclination to criticize string theory may therefore be justified.
How finite is string theory!
One criticism that has arisen largely since Smolin's The Trouble with Physics
is the notion that string theory isn't necessarily a finite theory. Remember
that this is one of the key features in support of string theory: It removes the
infinities that arise when you try to apply quantum physics directly to
problems.
As Smolin describes things, this belief in string theory finiteness is largely
based on a 1992 proof performed by Stanley Mandelstam, in which
Mandelstam only proved that the first term of string theory (remember that
string theory is an equation made up of an infinite series of mathematical
terms) was finite. It has since been proved for the second term, as well.
Chapter 17: Taking a Closer Look at the String Theory Controversy j/j
Still, even if every individual term is finite, string theory currently is written
in a form (like quantum field theory) that has an infinite number of terms.
Even if each term is finite, it's possible that the sum of all of the terms will
yield an infinite result. Because infinities are never witnessed in our universe,
this would mean that string theory doesn't describe our universe.
The fact that string theory finiteness hasn't been proved isn't a flaw in string
theory. The fact that most string theorists thought that it had been proved
finite when it wasn't is the flaw — not necessarily a flaw in string theory itself,
but a flaw in the very way these scientists are practicing their science. The
bigger issue at stake in this particular criticism is one of precision and
intellectual honesty.
A String Theory Rebuttal
In the light of all of these criticisms, many of which have some measure of
validity or logic to them, you may be wondering how anyone could continue
working on string theory. How could some of the most brilliant physicists in
the world devote their careers to exploring a field that is apparently a house
of cards?
The short answer, stated in various forms by many string theorists over the
years, is that they find it hard to believe that such a beautiful theory would
not apply to the universe. String theory describes all of the behavior of the
universe from certain fundamental principles as the vibrations of 1-dimensional
strings and compactification of extra dimensional geometries, and can be
used in some simplified versions to solve problems that have meaning to
physicists, such as black hole entropy.
Most string theorists are able to dismiss the idea that string theory should
be further along than it is. String theory does, after all, explore energies and
sizes beyond our current technology to test. And, even in cases where
experiment can guide theory, there are cases where 30 years was not enough
time.
The theory of light took much longer than 30 years to develop. In the late
1600s, Newton described light as tiny particles. In the 1800s, experiments
revealed that it traveled as waves. In 1905, Einstein proposed the quantum
principles that led to wave-particle duality, which in turn resulted in the
theory of quantum electrodynamics in the 1940s. In other words, the rigorous
physical examination of light traces a path from Newton through to Feynman
that covers about 250 years, filled with many false leads along the way.
And quantum electrodynamics is a quantum field theory, which means it has
infinite solutions unless it goes through a process of renormalization. The
fact that string theory may also be infinite isn't seen as a big deal, because
312 Part V: Wnat tne 0ther Gu V s Sa V : Criticisms and Alternatives _
the existing theory is definitely infinite. (Although, again, one of the
motivations of string theory was to remove the infinities.)
For that matter, it took more than 1,500 years for heliocentric models of the
Earth's motion to be accepted over geocentric models, even though anyone
could look up at the sky! It's only because our modern world moves so fast
that we feel we need quick and easy answers to something as simple as the
fundamental nature of the universe.
As mentioned earlier, neither side has won the debate (or "string wars")
yet, but many feel that the very fact that the debate is taking place is, on the
whole, good for science. And those who don't — well, they're probably part
of a groupthink cult of string theorists.
Chapter 18
Loop Quantum Gravity: String
Theory's Biggest Competitor
In This Chapter
Seeing how loop quantum gravity is more focused than string theory
Knowing what predictions loop quantum gravity makes
Evaluating the similarities between loop quantum gravity and string theory
T
■ hough string theory is often promoted as the "only consistent theory of
P quantum gravity" (or something along those lines), some would disagree
with this categorization. Foremost among them are the researchers in a field
known as loop quantum gravity (sometimes abbreviated LQG). I discuss other
approaches to quantum gravity in Chapter 19.
In this chapter, I introduce you to loop quantum gravity, an alternative theory
of quantum gravity. As string theory's major competitor, loop quantum gravity
hopes to answer many of the same questions by using a different approach.
I start by describing the basic principles of loop quantum gravity and then
present some of the major benefits of this approach over string theory. I lay
out some of the preliminary predictions of loop quantum gravity, including
possible ways to test it. Finally, I consider whether loop quantum gravity has
the same fundamental flaws that may bring down string theory.
Taking the Loop: Introducing Another
Road to Quantum Gravity
Loop quantum gravity is string theory's biggest competitor. It gets less press
than string theory, in part because it has a fundamentally more limited goal: a
quantum theory of gravity. Loop quantum gravity performs this feat by trying
to quantize space itself — in other words, treat space like it comes in small
chunks.
316 Part V: What the 0ther Guys Say: Critic ' sms and Alternatives _
In contrast, string theory starts with methods of particle physics and
frequently hopes to not only provide a method of creating a quantum theory
of gravity, but also explain all of particle physics, unifying gravity with the
other forces at the same time. Oh, and it predicts extra dimensions, which is
very cool!
It's no wonder that loop quantum gravity has more trouble getting press.
The great background debate
The key insight of quantum physics is that some quantities in nature come
in multiples of discrete values, called quanta. This principle has successfully
been applied to all of physics, except for gravity. This is the motivation for
the search for quantum gravity.
Alternately, the key insight from general relativity is that space-time is a
dynamic entity, not a fixed framework. String theory is a background-
dependent theory (built on a fixed framework; see Chapter 17 for more on
this), so it doesn't currently account for the dynamic nature of space-time at
the heart of relativity.
According to the LQG researchers, a theory of quantum gravity must be
background-independent, a theory that explains space and time instead of
being plugged into an already-existing space-time stage. No background-
dependent theory can ever yield general relativity as a low-energy
approximation.
Loop quantum gravity tries to achieve this goal by looking at the smooth
fabric of space-time in general relativity and contemplating the question
of whether, like regular fabric, it might be made up of smaller fibers woven
together. The connections between these quanta of space-time may yield a
background-independent way of looking at gravity in the quantum world.
What is looping anyway!
Loop quantum gravity's key insight is that you can describe space as a field;
instead of a bunch of points, space is a bunch of lines. The loop in loop
quantum gravity has to do with the fact that as you view these field lines
(which don't have to be straight lines, of course), they can loop around and
through each other, creating a spin network. By analyzing this network of
space bundles, you can supposedly extract results that are equivalent to the
known laws of physics.
_ Chapter 18: Loop Quantum Gravity: String Theory's Biggest Competitor 3 * w^
The foundation of LQG took place in 1986, when Abhay Ashtekar rewrote
general relativity as a series of field lines instead of a grid of points. The
result turns out not only to be simpler than the earlier approach, but is
similar to a gauge theory.
There's one problem, though: Gauge theories are background-dependent
theories (they are inserted into a fixed space-time framework), but that won't
work, because the field lines themselves represent the geometry of space.
You can't plug the theory into space if space is already part of the theory!
In order to proceed, physicists working in this area had to look at quantum
field theory in a whole new way so it could be approached in a background-
independent setting. Much of this work was performed by Ashtekar, Lee
Smolin, Ted Jacobson, and Carlo Rovelli, who can reasonably be considered
among the fathers of loop quantum gravity.
As LQG developed, it became clear that the theory represented a network of
connected quantum space bundles, often called "atoms" of space. The failure
of previous attempts to write a quantum theory of gravity was that space-
time was treated as continuous, instead of being quantized itself. The
evolution of these connections is what provides the dynamic framework of
space (although it has yet to be proved that loop quantum gravity actually
reduces to the same predictions as those given by relativity).
Each atom of space can be depicted with a point (called a node') on a certain
type of grid. The grid of all of these nodes, and the connections between
them, is called a spin network. (Spin networks were originally developed by
Oxford physicist Roger Penrose back in the 1970s.) The graph around each
node can change locally over time, as shown in Figure 18-1 (which shows the
initial state [a] and the new state it changes into [b]). The idea is that the
sum total of these changes will end up matching the smooth space-time
predictions of relativity on larger scales. (That last bit is the major part that
has yet to be proved.)
3 # v Part V: Wnat tne 0ther Gu V s Sa V : Criticisms and Alternatives _
Now, when you look at these lines and picture them in three dimensions, the
lines exist inside of space — but that's the wrong way to think about it. In
LQG, the spin network with all of these nodes and grid lines, the entire spin
network, is actually space itself. The specific configuration of the spin network
is the geometry of space.
The analysis of this network of quantum units of space may result in more
than physicists bargained for, because recent studies have indicated that
the Standard Model particles may be implicit in the theory. This work has
largely been pioneered by Fotini Markopoulou and work by the Australian
Sundance O. Bilson-Thompson. In Bilson-Thompson's model, the loops may
braid together in ways that could create the particles, as indicated in Figure
18-2. (These results remain entirely theoretical, and it remains to be seen
how they work into the larger LQG framework as it develops, or whether they
have any physical meaning at all.)
Chapter 18: Loop Quantum Gravity: String Theory's Biggest Competitor j//
Making Predictions With
Loop Quantum Gravity
Loop quantum gravity makes some definite predictions, which may mean
that it could be tested well before string theory can be. As string theory's
popularity is being brought into question, the amount of research into LQG
may end up growing.
Gravity exists (Duh!)
Oddly enough, because LQG was born out of general relativity, one question
has been whether science can get general relativity back out of the theory.
In other words, can scientists use loop quantum gravity to actually match
Einstein's classical theory of gravity on large scales? The answer is: yes, in
some special cases (as does string theory).
For example, work by Carlo Rovelli and his colleagues has shown that LQG
contains gravitons, at least in the low-energy version of the theory, and also
that two masses placed into the theory will attract each other in accord
with Newton's law of gravity. Further theoretical work is needed to get solid
correlations between LQG and general relativity.
Black holes contain only so much space
Loop quantum gravity's major success has been in matching the Bekenstein
prediction of black hole entropy as well as the Hawking radiation predictions
(both described in Chapter 9). As mentioned in Chapters 11 and 14, string
theory has been able to make some predictions about special types of black
holes, which is also consistent with the Bekenstein-Hawking theories. So,
at the very least, if scientists are able to create miniature black holes in the
Large Hadron Collider and observe Hawking radiation, then it would certainly
not rule out either of the theories.
However, the picture given by LQG is very different from that of classical
black holes. Instead of an infinite singularity, the quantum rules say there's
only so much space inside of the black hole. Some LQG theorists hope they
can predict tiny adjustments to Hawking's theory that, if experimentally
proven true, would support LQG above string theory.
jl O P art V: What the Other Guys Say: Criticisms and Alternatives _
One prediction is that instead of a singularity, the matter falling into a black
hole begins expanding into another region of space-time, consistent with
some earlier predictions by Bryce DeWitt and John Archibald Wheeler. In
fact, singularities at the big bang are also eliminated, providing another
possible eternal universe model. (For more eternal universe models, see
Chapter 14.)
Gamma ray burst radiation
travels at different speeds
Many of the experiments from Chapter 12, which could test whether the
speed of light varies, would also be consistent with loop quantum gravity. For
example, it's possible that gamma ray burst radiation doesn't all travel at the
same speed, like classical relativity predicts. As the radiation passes through
the spin network of quantized space, the high-energy gamma rays would
travel slightly slower than the low-energy gamma rays. Again, these effects
would be magnified over the vast distances traveled to possibly be observed
by the Fermi telescope.
Finding Fatfor and FtaW With
Loop Quantum Gravity
As with string theory, loop quantum gravity is passionately embraced by
some physicists and dismissed by others. The physicists who study it believe
that the predictions (described in the preceding section) are far better
than those made by string theory. One major argument in support of LQG
is that it's seen by its adherents as a finite theory, meaning that the theory
itself doesn't inherently admit infinities. These same researchers also tend
to dismiss the flaws as being the product of insufficient work (and funding)
devoted to the theory. String theorists, in turn, view them as much a victim of
"groupthink" as critics view string theorists.
The benefit of a finite theorem
One major benefit of loop quantum gravity is that the theory has been proved
finite in a more definitive sense than string theory has. Lee Smolin, one of
the key (and certainly most high profile) researchers of LQG, describes in
his book The Trouble with Physics three distinct ways that the theory is finite
(with string theorist objections in parentheses):
_ Chapter 18: Loop Quantum Gravity: String Theory's Biggest Competitor 3 * •
W The areas and volumes in loop quantum gravity are always in finite,
discrete units. (String theorists would say this isn't a particularly
meaningful form of finiteness.)
j-" In the Barrett-Crane model of loop quantum gravity, the probabilities for
a quantum geometry to evolve into different histories are always finite.
(This sounds just like unitarity, which is a property of string theory and
all quantum field theories.)
u* Including gravity in a loop quantum gravity theory that contains matter
theory, like the Standard Model, involves no infinite expressions. If
gravity is excluded, you have to do some tinkering to avoid them. (String
theorists believe this claim is premature and that there are substantial
problems with the proposed LQG models that yield this result.)
As I explain in Chapter 17, some questions exist (largely brought up by loop
quantum gravity theorists) about whether string theory is actually finite —
or, more specifically, over whether it has been rigorously proved finite. From
the theoretical side of things, the loop quantum gravity people view this
uncertainty as a major victory over string theory. (String theorists would
argue that the statements above still don't prove that LQG can't result in an
infinite solution when experimental data is put into the theory.)
Spending some time focusing on the ftaWs
Many of the flaws in loop quantum gravity are the same flaws in string
theory. Their predictions generally extend into realms that aren't quite
testable yet (although LQG is a bit closer to being able to be experimentally
tested than string theory probably is). Also, it's not really clear that loop
quantum gravity is any more falsifiable than string theory. For example, the
discovery of supersymmetry or extra dimensions won't disprove loop
quantum gravity any more than the failure to detect them will disprove
string theory. (The only discovery that I think LQG would have a hard time
overcoming would be if black holes are observed and Hawking radiation proves
to be false, which would be a problem for any quantum gravity theory,
including string theory.)
The biggest flaw in loop quantum gravity is that it has yet to successfully
show that you can take a quantized space and extract a smooth space-time
out of it. In fact, the entire method of adding time into the spin network
seems somewhat contrived to some critics, although whether it's any more
contrived than the entirely background-dependent formulation of string
theory remains to be seen.
The quantum theory of space-time in loop quantum gravity is really just a
quantum theory of space. The spin network described by the theory cannot
yet incorporate time. Some, such as Lee Smolin, believe that time will prove
j20 Part V: Wnat tne 0ther Gu V s Sa V : Criticisms and Alternatives _
to be a necessary and fundamental component of the theory, while Carlo
Rovelli believes that the theory will ultimately show that time doesn't really
exist, but is just an emergent property without a real existence on its own.
These and other disputes over the meaning of time are addressed in Chapter 16.
So Are These Tu/o Theories the Same
u/ith Different Names}
One viewpoint is that both string theory and loop quantum gravity may
actually represent the same theory approached from different directions.
The parallels between the theories are numerous:
v* String theory began as a theory of particle interactions, but was shown
to contain gravity. Loop quantum gravity began as a theory of gravity,
but was shown to contain particles.
j-" In string theory, space-time can be viewed as a mesh of interacting
strings and branes, much like the threads of a fabric. In loop quantum
gravity, threads of space are woven together, creating the apparently
"smooth" fabric of space-time.
v* Some string theorists believe the compactified dimensions represent a
fundamental quantum unit of space, while LQG starts with units of space
as an initial requirement.
V Both theories (provided certain assumptions are made) calculate the
I same entropy for black holes.
One way to view the differences is that string theory, which began by
applying principles from particle physics, may point toward a universe in
which space-time emerges from the behavior of these fundamental strings.
LQG, on the other hand, began by applying general relativity principles and
results in a world where space-time is fundamental, but matter and gravity
may emerge from the behavior of these fundamental units.
At one time, Lee Smolin was one of the major supporters of the viewpoint
that string theory, M-theory, and loop quantum gravity were different
approximations of the same underlying fundamental theory. Over the last
decade, he has become largely disillusioned with string theory (at least
compared to his earlier conciliatory stance), becoming a prominent advocate
of pursuing other avenues of inquiry.
Some string theorists believe that the methods used by LQG will eventually
be carried over to string theory, allowing for a background-independent
version of string theory. This is very probable, especially given that the
string theory landscape seems capable of absorbing virtually any viable
theory and incorporating it as a part of string theory.
.Chapter 18: Loop Quantum Gravity: String Theory's Biggest Competitor 3^- /
Despite the possible harmony between the two fields, at the moment they are
competitors for research funding and attention. String theorists have their
conferences, and loop quantum gravity people have their conferences, and
rarely shall the two conferences meet. (Except for Lee Smolin, who seems to
have rather enjoyed flitting over to the string theory side of things over the
years.) All too often, the groups seem unable to speak to each other in any
meaningful way (see the nearby sidebar, "The 'Big Bang' breakup").
Part of the problem is one of sociology. Many string theorists, even in
research papers, use phrases that make it clear they consider string theory
to not only be their preferred theory, but to be the only (or, in cases where
they're being more generous, the "most promising") theory of quantum
gravity. By doing this, they often dismiss LQG as even being an option.
Some string theorists have indicated in interviews that they are completely
unaware of any viable alternatives to string theory! (This is because string
theorists aren't yet convinced that the alternatives are actually viable.)
Hopefully, these physicists will find a way to work together and use their
results and techniques in ways that provide real insights into the nature of
our own universe. But so far, loop quantum gravity, like string theory, is still
stuck on the drawing board.
The "Big Bang" breakup
The conflict between loop quantum gravity and
string theory enthusiasts made it into popu-
lar culture in an episode of the CBS television
sitcom The Big Bang Theory, which focuses on
two physicist roommates, Leonard and Sheldon.
In the second episode of the second season,
Leonard has begun a relationship with a physicist
colleague, Leslie Winkle, a rival of Sheldon (or
"nemesis," as he thinks of her). Leslie Winkle,
you see, is a researcher in loop quantum gravity,
while Sheldon is a string theorist.
In the climactic scene of the episode, Sheldon
and Leslie get into a "string war" of their own,
slinging theoretical physics barbs at each
other. Their conflict is over which theory —
loop quantum gravity or string theory — has the
probability of successfully achieving a
quantum theory of gravity. The argument ends
in Leonard being placed in the middle, being
forced to point out that they are two untested
theories of quantum gravity, so he has no way to
choose. Leslie is shocked and appalled by this
response, immediately ending the relationship
with Leonard.
Although this is obviously played up for comedy
purposes, among the physics community the
funniest thing a bout it was how much truth there
actually was in the scenario. When physicists
get into passionate debates about loop
quantum gravity versus string theory, all too
often the first casualty seems to be reasonable
discourse.
322 Part V: Wnat tne 0ther Gu V s Sa V : Criticisms and Alternatives _
Chapter 19
Considering Other Ways to
Explain the Universe
In This Chapter
Some physicists are working in areas other than string theory — honest!
Working around the need for a theory of quantum gravity
Seeking new mathematical approaches while solving string theory problems
■ n the event that string theory proves false, or that there is no "theory
*5 of everything" at all, there are still some unexplained phenomena in the
universe that require explanation. These issues mostly lie in the realm of
cosmology, such as the flatness problem, dark matter, dark energy, and the
details of the early universe.
Even though string theory is currently the dominant path being explored to
answer most of these problems, some physicists have begun looking in other
directions, beyond the loop quantum gravity described in Chapter 18. These
rebels (and, at times, outcasts) have refused, in many cases, to stick with the
mainstream theoretical community in adopting the principles of string theory
and have proposed new directions of inquiry that are, at times, extremely
radical — though possibly no more radical, in their own ways, than string
theory was in the 1970s.
In this chapter, I explain some of the alternative approaches that physicists
are looking into in an effort to explain the problems that physicists want to
resolve. First, I explore some alternate quantum gravity theories, none of
which are quite as fully developed as either string theory or loop quantum
gravity. Next, I show you how physicists have suggested modifying the
existing law of general relativity to take into account the facts that don't fit
with Einstein's original model. It's possible that some of the ideas from this
chapter will ultimately be incorporated into string theory, or perhaps take its
place entirely.
3 24 1 Part V: Wnat tne 0ther Guvs Sav: Criticisms and Alternatives _
Taking Other Roads to Quantum Gravity
Though string theorists like to point out that theirs is the most developed
theory to unite general relativity and quantum physics (at times they even
seem clueless that alternatives exist), sometimes it seems like nearly every
physicist has come up with some plan to combine the two — they just don't
have the support that string theorists have.
Most of these alternate theories start with the same idea as loop quantum
gravity — that space is made up of small, discrete units that somehow work
together to provide the space-time that we all know and love (relatively
speaking, that is). Despite the fact that scientists don't know much about
these units of space, some theorists can analyze how they might behave and
use that information to generate useful models.
Here are some examples of these other quantum gravity approaches:
K" Causal dynamical triangulations (CDT): CDT models space-time as
being made up of tiny building blocks, called 4-simplices, which are
identical and can reconfigure themselves into different curvature
configurations.
(<" Quantum Einstein gravity (or "asymptotic safety"): Quantum Einstein
gravity assumes that there's a point where "zooming in" on space-time
stops increasing the force of gravity.
(<" Quantum graphity: In the quantum graphity model, gravity didn't exist
in the earliest moments of the universe because space itself doesn't
exist on the small length and high energy scales involved in the early
universe.
v" Internal relativity: This model predicts that you can start with a
random distribution of quantum spins and get the laws of general
relativity to come out of it.
Of course, any of these approaches could advance either string theory or
loop quantum gravity, instead of leading off in a new direction. Some of the
principles may prove fruitful, but only when applied in the framework of one
of the other theories. Only time will tell what insights, if any, come out of them
and if they can be applied to give meaningful results.
Causal dynamical triangulations (CDT):
If you'Oe got the time, Vve got the space
The causal dynamical triangulations approach consists of taking tiny
building blocks of space, called 4-simplices (sort of like multidimensional
triangles), and using them to construct the space-time geometry. The result
.Chapter 19: Considering Other Ways to Explain the Universe ^23
is a sequence of geometric patterns that are causally related in a sequence
where one construction follows another (in other words, one pattern causes
the next pattern). This system was developed by Renate Loll of Utrecht
University in the Netherlands, and also by colleagues Jan Ambjorn and Jerzy
Jurkiewicz.
One of the most important aspects of CDT is that time becomes an essential
component of space-time, because Loll includes the causal link as a crucial
part of the theory. Relativity tells us that time is distinctly different from
space (as mentioned in Chapter 13, the time dimension has a negative in
front of it in relativity), but Stephen Hawking and others have suggested that
the difference between time and space could perhaps be ignored.
Loll then takes her causally linked configurations of 4-simplices and sums
over all possible configurations of the shapes. (Feynman used a similar
approach in quantum mechanics, summing over all possible paths to obtain
quantum physics results.) The result is classical space-time geometry!
If true, CDT shows that it's impossible to ignore the difference between space
and time. The causal link of changes in space-time geometry — in other words,
the "time" part of space-time — is absolutely necessary to get classical space-
time geometry that is governed by general relativity and matches what science
knows of standard cosmological models.
At the tiniest scales, though, CDT shows that space-time is only 2-dimensional.
The model turns into a fractal pattern, where the structures repeat themselves
at smaller and smaller scales, and there's no proof that real space-time
behaves that way.
CDT's biggest flaw in comparison to string theory is that it doesn't tell us
anything about where matter comes from, whereas matter arises naturally in
string theory from the interactions of fundamental strings.
Quantum Einstein gravity: Too small to tug
Quantum Einstein gravity, developed by Martin Reuter of the University of
Mainz in Germany, tries to apply the quantum physics processes that worked
on other forces to gravity. Reuter believes that at small scales, gravity may
have a cutoff point where its strength stops increasing. (This notion was
proposed by Steven Weinberg in the 1970s, under the more common name
"asymptotic safety.")
One reason to think that gravity stops increasing at small scales is that this is
what quantum field theory tells us the other forces do. At very small scales,
even the strong nuclear force drops to zero. This is called asymptotic freedom,
and its discovery earned David Gross, David Politzer, and Frank Wilczek
the 2004 Nobel Prize. The force of gravity wouldn't go to zero but rather to
326 Part V: Wnat tne 0ther Guys Say: Cr ' tic ' sms and Alternatives _
some finite strength (stronger than we usually see), and this idea is known as
asymptotic safety.
Weinberg and others weren't able to pursue the idea at the time because
the mathematical tools to calculate the cutoff point for gravity in general
relativity didn't exist until Reuter developed them in the 1990s. Though the
method is approximate, Reuter has a great deal of confidence.
Quantum Einstein gravity, like CDT, comes up with a fractal pattern to small-
scale space-time, and the number of dimensions drops to two. Reuter himself
has noted that this could mean that his approach is fundamentally equivalent
to CDT, because they both have these rather distinctive predictions at small
scales.
The idea of asymptotic safety is really a very conservative solution to the
problem of quantum gravity. Unlike the other approaches that introduce
some radically new physics that would take over from general relativity at
high energies (or equivalently at short distances), it proposes a well-defined
strongly interacting theory of gravity at high energies in which the usual
general relativity is simply augmented by some extra interactions for the
graviton.
Quantum qmphity: Disconnecting nodes
Quantum graphity has been developed by Fotini Markopoulou of the
Perimeter Institute. In some ways, this is loop quantum gravity taken to its
extreme — at extremely high energies all that exists is the network of nodes.
This model is based on a suggestion by John Archibald Wheeler about a
pre-geometric phase to the universe, which Markopoulou takes literally. The
nodes in the pre-geometric phase would all touch each other, but as the
universe cooled, they would disconnect from each other and become
separated, resulting in the space that we see today. (Physicists working on
string theory have also found this sort of pre-geometric phase, so it's not
unique to Markopoulou's approach.)
It's also possible that this could explain the horizon problem, the problem
that distant parts of the universe seem to be the same temperature. In the
quantum graphity model, all points used to be in direct contact, so inflation
proves to be unnecessary. (See Chapter 9 for more about the horizon
problem and how inflation solves it.) At present, inflation is a much more
well-defined theory, but Markopoulou is working on developing quantum
graphity to compete with it.
.Chapter 19: Considering Other Ways to Explain the Universe 3» /
The Perimeter Institute
If you follow theoretical physics, it isn't long
until you hear about the Perimeter Institute
for Theoretical Physics, located in Waterloo,
Ontario, Canada. The Perimeter Institute was
founded in 1999 by Mike Lazaridis, who was
founder and co-CEO of Research in Motion,
the makers of the BlackBerry handheld device.
Lazaridis decided to help foster research and
innovation in Canada by starting the Perimeter
Institute, which is devoted purely to theoretical
physics research.
Many of the prominent critics of string theory
who are working on other approaches — Lee
Smolin, John Moffat, Fotini Markopoulou, and
others — call it home, so it's easy to believe
that the Perimeter Institute seeks out anti-string
theorists. In fact, their current director is Neil
Turok, a cosmologist and co-creator of the
ekpyrotic model, which is based on string theory
principles. The Perimeter Institute achieved
quite a coup by hiring Stephen Hawking as a
Distinguished Research Chair, followed by a
slew of other prominent physicists.
The Perimeter Institute's goal is to foster
innovation, and the physicists work in a number
of areas: cosmology, particle physics, quantum
foundations, quantum gravity, quantum
information theory, and superstring theory.
It's one of the only places where string
theorists and leaders in other quantum gravity
approaches regularly work together in one
institute. More information on the Perimeter
Institute can be found at www. perimeter
institute. ca.
Internal relativity: Spinning
the universe into existence
The final quantum gravity model, internal relativity, may be the most
ambitious, because Olaf Dreyer of MIT believes that a random distribution of
quantum spins may end up resulting in our whole universe. For this to work,
Dreyer considers the view of observers inside the system. The approach has
shown that these observers would witness some aspects of special relativity,
such as time dilation and length contraction, but Dreyer is still working on
getting general relativity out of the equations. (Isn't everybody?)
The space-time and matter are a result of the excitations of the system, which
is one reason Dreyer is hopeful. He believes that the reason quantum physics
yields an incorrect prediction for the cosmological constant is because of a
split between space-time and matter. Internal relativity links the two concepts,
so the calculations have to be performed differently.
Dreyer has predicted that his model would show no gravity waves in the
cosmic microwave background radiation (CMBR), while inflation theory
would result in CMBR gravity waves. It is hoped that the Planck satellite will
be able to detect any gravity waves in the CMBR — or not detect them, as
Dreyer's theory predicts.
j2o P art ^ : What the Other Guys Say: Criticisms and Alternatives _
Nertton and Einstein Don't Make Alt the
Rules: Modifying the Law of Gravity
Instead of trying to develop theories of quantum gravity, some physicists are
looking at the existing law of gravity and trying to find specific modifications
that will make it work to explain the current mysteries of cosmology.
These efforts are largely motivated by attempts to find alternatives to the
cosmological theories of inflation, dark matter, or dark energy.
These approaches don't necessarily resolve the conflicts between quantum
physics and general relativity, but in many cases they make the conflict less
important. The approaches tend to result in singularities and infinities falling
out of the theories, so there just isn't as much need for a theory of quantum
gravity.
Doubly special relativity (DSR): Twice
as many limits as ordinary relativity
One intriguing approach is doubly special relativity or deformed special
relativity (abbreviated as DSR either way you slice it), originally developed
by Giovanni Amelino-Camelia. In special relativity, the speed of light is
constant for all observers. In DSR theories, all observers also agree on one
other thing — the distance of the Planck length.
In Einstein's relativity, the constancy of the speed of light places an upper
speed limit on everything in the universe. In DSR theories, the Planck length
represents a lower limit on distance. Nothing can go faster than the speed of
light, and nothing can be smaller than a Planck length. The principles of DSR
may be applicable to various quantum gravity models, such as loop quantum
gravity, though so far there's no proof for it.
Modified Newtonian dynamics (M0A1D):
Disregarding dark matter
Some physicists aren't comfortable with the idea of dark matter and have
proposed alternative explanations to resolve the problems that make
physicists believe dark matter exists. One of these explanations, which
involves looking at gravity in a new way on large scales, is called modified
Newtonian dynamics (MOND).
.Chapter 19: Considering Other Ways to Explain the Universe J2y
The basic premise of MOND is that at low values, the force of gravity doesn't
follow the rules laid out by Newton more than 300 years ago. The relationship
between force and acceleration in these cases may turn out not to be exactly
linear, and MOND predicts a relationship that will yield the results observed
based on only the visible mass for galaxies.
In Newtonian mechanics (or, for that matter, in general relativity, which
reduces to Newtonian mechanics at this scale), the gravitational relationships
between objects are precisely defined based on their masses and the distance
between them. When the amount of visible matter for galaxies is put into
these equations, physicists get answers that show that the visible matter
just doesn't produce enough gravity to hold the galaxies together. In fact,
according to Newtonian mechanics, the outer edges of the galaxies should
be rotating much faster, causing the stars farther out to fly away from the
galaxy.
Because scientists know the distances involved, the assumption is that
somehow the amount of matter has been underestimated. A natural response
to this (and the one that most physicists have adopted) is that there must be
some other sort of matter that isn't visible to us: dark matter.
There is one other alternative — the distances and matter are correct, but
the relationship between them is incorrect. MOND was proposed by Israeli
physicist Mordehai Milgrom in 1981 as a means of explaining the galactic
behavior without resorting to dark matter.
Most physicists have ruled MOND out, because the dark matter theories
seem to fit the facts more closely. Milgrom, however, has not given up, and in
2009 he made predictions about slight variations in the path of planets based
on his MOND calculations. It remains to be seen if these variations will be
observed.
Variable speed of light (USD: Light
used to travel eVen faster
In two separate efforts, physicists have developed a system where the speed
of light actually would not be constant, as a means of explaining the horizon
problem without the need of inflation. The earliest system of the variable
speed of light (VSL) was proposed by John Moffat (who later incorporated the
idea into his modified gravity theory), and a later system was developed by
Joao Magueijo and Andreas Albrecht.
33 Part V: Wnat the 0ther Guvs Sa V : Criticisms and Alternatives _
Proving dark matter wrong?
In August 2008, a group of astrophysicists
published a paper called "A Direct Empirical
Proof of the Existence of Dark Matter." The
"proof" they speak of came from an impact
between two galaxy clusters. Using NASA's
Chandra X-Ray Observatory, they were able
to see gravitational tensing (the gravity of the
collision caused light to bend, kind of how light
bends when it passes through a lens), which let
them determine the center of the collision. The
center of the collision did not match the center
of the visible matter. In other words, the center
of gravity and the center of visible matter didn't
match. That's pretty conclusive evidence for
there being nonvisible matter, right?
In the world of theoretical physics, nothing
is quite that easy these days. By September,
physicist John Moffat and others were beg inning
to cast doubt on whether dark matter was
the only explanation. Using his own modified
gravity (MOG) theory, Moffat performed a
calculation on a simplified 1-dimensional
version of the collision.
Most physicists accept the NASA findings,
including more recent findings from WMAP
and other observations, as conclusive evidence
that dark matter exists. But there remain those
who are unconvinced and search for other
explanations.
The horizon problem is based on the idea that distant regions of the universe
couldn't communicate their temperatures because they are so far apart light
hasn't had time to get from one to the other. The solution proposed by
inflation theory is that the regions were once much closer together, so they
could communicate (see Chapter 9 for more on this).
In VSL theories, another alternative is proposed: The two regions could
communicate because light traveled faster in the past than it does now.
Moffat proposed his VSL model in 1992, allowing for the speed of light in the
early universe to be very large — about 100,000 trillion trillion times the
current values. This would allow for all regions of the observable universe to
easily communicate with each other.
To get this to work out, Moffat had to make a conjecture that the Lorentz
invariance — the basic symmetry of special relativity — was somehow
spontaneously broken in the early universe. Moffat's prediction results in a
period of rapid heat transfer throughout the universe that results in the same
effects as an inflationary model.
In 1998, physicist Joao Magueijo came up with a similar theory, in
collaboration with Aldreas Albrecht. Their approach, developed without any
knowledge of Moffat's work, was very similar — which they acknowledged
upon learning of it. This work was published a bit more prominently than
Moffat's (largely because they were more stubborn about pursuing
.Chapter 19: Considering Other Ways to Explain the Universe jj /
publication in the prestigious Physical Review D, which had rejected Moffat's
earlier paper). This later work has inspired others, such as Cambridge physi-
cist John Barrow, to begin investigating this idea.
One piece of support for VSL approaches is that recent research by John
Webb and others has indicated that the fine-structure constant may not have
always been constant. The fine-structure constant is a ratio made up from
Planck's constant, the charge on the electron, and the speed of light. It's a
value that shows up in some physical equations. If the fine-structure constant
has changed over time, then at least one of these values (and possibly more
than one) has also been changing.
The spectral lines emitted by atoms are defined by Planck's constant.
Scientists know from observations that these spectral lines haven't changed,
so it's unlikely that Planck's constant has changed. (Thanks to John Moffat
for clearing that up.) Still, any change in the fine-structure constant could be
explained by varying either the speed of light or the electron charge (or both).
Physicists Elias Kiritsis and Stephon Alexander independently developed VSL
models that could be incorporated into string theory, and Alexander later
worked with Magueijo on refining these concepts (even though Magueijo is
critical of string theory's lack of contact with experiment).
These proposals are intriguing, but the physics community in general remains
committed to the inflation model. Both VSL and inflation require some strange
behavior in the early moments of the universe, but it's unclear that inflation is
inherently more realistic than VSL. It's possible that further evidence of varying
constants will ultimately lead to support of VSL over inflation, but that day
seems a long way off, if it ever happens.
Modified qvatfty (MOG): The bigger
the distance, the greater the gravity
John Moffat's work in alternative gravity has resulted in his modified
gravity (MOG) theories, in which the force of gravity increases over distance,
and also the introduction of a new repulsive force at even larger distances.
Moffat's MOG actually consists of three different theories that he has
developed over the span of three decades, trying to make them simpler and
more elegant and more accessible for other physicists to work on.
This work began in 1979, when Moffat developed nonsymmetric gravitational
theory (NGT), which extended work that Einstein tried to apply to create a
unified field theory in the context of a non-Riemannian geometry. The work
had failed to unify gravity and electromagnetics, like Einstein wanted, but
Moffat believed that it could be used to generalize relativity itself.
33 2 Part V: Wnat tne 0ther Gu V s Sa V : Criticisms and Alternatives _
Over the years, NGT ultimately proved inconclusive. It was possible that its
predictions (such as the idea that the sun deviated from a perfectly spherical
shape) was incorrect or that the deviation was too small to be observed.
In 2003, Moffat developed an alternative with the unwieldy name Metric-Skew-
Tensor Gravity (MSTG). This was a symmetric theory (easier to deal with),
which included a "skew" field for the nonsymmetric part. This new field was,
in fact, a fundamentally new force — a fifth fundamental force in the universe.
Unfortunately, this theory remained too mathematically complicated in
the eyes of many, so in 2004 Moffat developed Scalar-Tensor-Vector Gravity
(STVG). In STVG, Moffat again had a fifth force resulting from a vector field
called a phion field. The phion particle was the gauge boson that carried the
fifth force in the theory.
According to Moffat, all three theories give essentially the same results for
weak gravity fields, like those we normally observe. The strong gravitational
fields needed to distinguish the theories are the ones that always give
scientists problems and have motivated the search for quantum gravity
theories in the first place. They can be found at the moment of the big bang
or during the stellar collapses that may cause black holes.
There are indications that STVG yields results very similar to Milgrom's
MOND theory (refer to the earlier section "Modified Newtonian dynamics
(MOND): Disregarding dark matter" for a fuller explanation of MOND). Moffat
has proposed that MOG may actually explain dark matter and dark energy,
and that black holes may not actually exist in nature.
While these implications are amazing, the work is still in the very preliminary
stages, and it will likely be years before it (or any of the other theories)
is developed enough to have any hope of seriously competing with the
entrenched viewpoints.
RevOritinq the Math Books and Physics
Books at the Same Time
Revolutions in physics have frequently had an assist from revolutions in
mathematics years before. One of the problems with string theory is that it
has advanced so quickly that the mathematical tools didn't actually exist.
Physicists have been forced (with the aid of some brilliant mathematicians)
to develop the tools as they go.
.Chapter 19: Considering Other Ways to Explain the Universe 333
Einstein got help in developing general relativity from Riemannian geometry,
developed years earlier. Quantum physics was built on a framework of new
mathematical representations of physical symmetries, group representation
theory, as developed by the mathematician Hermann Weyl.
In addition to developing the physics needed to address problems of
quantum gravity, some physicists and mathematicians have tried to focus
on developing whole new mathematical techniques. The question remains,
though, how (and if) these techniques could be applied to the theoretical
frameworks to get meaningful results.
Compute this: Quantum information theory
One technique that is growing in popularity as a means of looking at the
universe is quantum information theory, which deals with all elements in the
universe as pieces of information. This approach was originally proposed
by John Archibald Wheeler with the phrase "It from bit," indicating that all
matter in the universe can be viewed as essentially pieces of information. (A
bit is a unit of information stored in a computer.)
Some of the leaders in this approach are Fotini Markopoulou of the Perimeter
Institute and Seth Lloyd of MIT, who approach the problem from rather
different directions. Markopoulou studies quantum gravity theories, while
Lloyd is best known for having figured out how to build a quantum computer.
(Quantum computers are like ordinary computers, but instead of using just
two bits for information storage, they use quantum physics to have a whole
host of in-between information. A quantum bit of information is called a
qubit?)
Overall, this approach basically treats the universe as a giant computer — in
fact, a universe-sized quantum computer. The major benefit of this system is
that, for a computer scientist, it's easy to see how random information sent
through a series of computations results in complexity growing over time.
The complexity within our universe could thus arise from the universe
performing logical operations — calculations, if you will — upon the pieces of
information (be they loops of space-time or strings) within the universe.
If you want to know more about quantum information theory, or quantum
computers for that matter, you can read about it in Seth Lloyd's 2006 physics
book, Programming the Universe: A Quantum Computer Scientist Takes on the
Cosmos, which should be accessible if you've followed the science in this
book.
336 Part V: What the 0ther Guys Say: Criticisms and Alternatives
Looking at relationships: Tutistor theory
For nearly four decades, the brilliant physicist Sir Roger Penrose has been
exploring his own mathematical approach — twistor theory. Penrose
developed the theory out of a strong general relativity approach (the theory
requires only four dimensions). Penrose maintains a belief that any theory
of quantum gravity will need to include fundamental revisions to the way
physicists think about quantum mechanics, something with which most
particle physicists and string theorists disagree.
One of the key aspects of twistor theory is that the relation between events
in space-time is crucial. Instead of focusing on the events and their resulting
relationships, twistor theory focuses on the causal relationships, and the
events become byproducts of those relationships.
If you take all of the light rays in space-time, it creates a twistor space, which
is the mathematical universe in which twistor theory resides. In fact, there
are some indications that objects in twistor space may result in objects and
events in our universe.
The major flaw of twistor theory is that even after all of these years (it was
originally developed in the 1960s), it still only exists in a world absent of
quantum physics. The space-time of twistor theory is perfectly smooth, so
it allows no discrete structure of space-time. It's a sort of anti-quantum
gravity, which means it doesn't provide much more help than general
relativity in resolving the issues that string theorists (or other quantum
gravity researchers) are trying to solve.
As with string theory, Penrose's twistor theory has provided some mathematical
insights into the existing theories of physics, including some that lie at the
heart of the Standard Model of particle physics.
Edward Witten and other string theorists have begun to investigate ways that
twistor theory may relate to string theory. One approach has been to have
the strings exist not in physical space, but in twistor space. So far, it hasn't
yielded the relationships that would provide fundamental breakthroughs in
either string theory or twistor theory, but it has resulted in great improvements
of calculational techniques in quantum chromodynamics.
Uniting mathematical systems:
MoncommutatiVe geometry
Another mathematical tool being developed is the noncommutative geometry of
French mathematician Alain Connes, a winner of the prestigious Fields Medal.
This system involves treating the geometry in a fundamentally new way, using
mathematical systems where the commutative principle doesn't hold.
.Chapter 19: Considering Other Ways to Explain the Universe 335
In mathematics, two quantities commute if operations on those quantities
work the same way no matter what order you treat them. Addition and
multiplication are both commutative because you get the same answer no
matter what order you add two numbers or multiply them.
However, mathematicians are a diverse bunch, and some mathematical
systems exist where addition and multiplication are defined differently, so
the order does matter. As weird as it sounds, in these systems multiplying 5
by 3 could give a different result than multiplying 3 by 5. (I don't recommend
using this excuse to argue with a teacher over the scores on a math test.) It's
probably not surprising to discover that these noncommutative mathematical
systems come up frequently in the bizarre world of quantum mechanics —
in fact, this feature is the mathematical cause of the uncertainty principle
described in Chapter 7.
The tools of noncommutative geometry have been used in many approaches,
but Connes seeks a more fundamental unification of algebra and geometry
that could be used to build a physical model where the conflicts are resolved
by features inherent in the mathematical system.
Noncommutative geometry has had some success, because the Standard
Model of particle physics seems to pop out of it in the simplest versions.
The goal of the committed mathematicians working with Connes is that they
will eventually be able to replicate all of physics (including possibly string
theory), though that is likely still a long way off. (Are you beginning to see a
pattern here?)
330 Part V: Wnat tne 0ther Gu y s Sav: Criticisms and Alternatives _
Part VI
The Part of Tens
The 5 th Wave
By Rich Tennant
\PRcX. MElW PREPARES TO PELIVER
[ HIS PAPER on STRING THEORY
In this part .
■ n these classic For Dummies Part of Tens chapters, I
•S offer some greater insights into what string theory
might accomplish and the people closest to it.
I explore ten concepts that physicists hope a "theory of
everything" will explain, whether or not string theory
turns out to be that theory.
I also give you some background on ten of the most
prominent string theorists working to show that string
theory is the way to unite quantum theory and general
relativity.
Chapter 20
Ten Questions a Theory of
Everything Should (Ideally)
Answer
In This Chapter
Hoping to unlock the secrets of the origin and end of the universe
Wondering why our universe has the parameters it does
Seeking explanations for dark matter, dark energy, and other mysteries
A\ ny "theory of everything" — whether it be string theory or something
V \ else — would need to answer some of the most difficult questions that
physics has ever asked. These questions are so difficult that the combined
efforts of the entire physics community have so far been unable to answer
them. Most physicists have, historically, believed that a theory of everything
would provide a unique reason why the universe is the way it is — as
opposed to the anthropic principle, which is based on our universe not being
unique. Many physicists today question whether there can ever be a single
theory that answers all of these questions.
In this chapter, I consider the questions of what started the universe,
including why the early universe had exactly the properties it had. This
includes the solutions to other questions of cosmology, such as the nature
of black holes, dark matter, and dark energy. I also explore the problem of
understanding what really happens in the strange realm of quantum physics.
Finally, I discuss the need for a fundamental explanation of time and a
reasonable look ahead at the end of the universe.
31*0
Part VI: The Part of Tens _
The Bia Bang: What Banged
(and Inflated)?
Currently, physics and cosmology tell us that the universe as we know it
started about 14 billion or so years ago, in a singularity at which the laws of
physics break down. Most scientists believe in a rapid inflation that occurred
moments afterward, expanding space rapidly. When the inflation period
slowed down, we entered into a period where space continued to expand at
the rate we see today (or a bit less, given dark energy's influences).
This breaks the question of the universe's origin into two parts:
v" What were the initial conditions that triggered the big bang?
v" What caused the repulsive gravity of the inflation era to end?
In Chapter 14, 1 offer some explanations for how string theory can solve these
questions. Even if string theory fails, any theory that attempts to expand
beyond the Standard Model of particle physics will need to tackle these
questions regarding the early moments of the universe.
Baryon Asymmetry: Why
Does Matter Exist?
After the big bang, raw energy was transformed into matter. If the energy of
the early universe had cooled into equal amounts of matter and antimatter,
these different forms of matter would have annihilated each other, leaving
no matter in the universe. Instead, there was substantially more matter than
antimatter, enough so that when all the antimatter had been annihilated by
matter, enough matter was left to make up the visible universe. This early
difference between matter and antimatter is called baryon asymmetry
(because regular matter, made up of baryons, is called baryonic matter).
The laws of physics provide no clear reason why the amounts of matter and
antimatter wouldn't have been equal, so presumably a theory of everything
would explain why the dense energy of the early universe tended to favor —
even if only by a little bit — matter over antimatter.
Chapter 20: Ten Questions a Theory of Everything Should (Ideally) Answer JU /
Hierarchy Issues: Why Are There Gaps in
Forces, Particles, and Energy Levels?
Most physicists, if they were to set out to create a universe, would have been
a bit more conservative with their resources than the forces at work in our
universe seem to have been. There are a wide range of force intensities,
ranging from the incredibly weak gravitational force to the strong nuclear
force that binds quarks together into protons and neutrons. The particles
themselves come in multiple varieties — far more varieties than we seem
to need — and each variety jumps by large multiples in size. Instead of a
smooth continuum of forces, particles, and energy, there are huge gaps.
A theory of everything should explain why these gaps exist and why they
exist where they do.
Fine-Tuning: Why Do Fundamental
Constants Hatfe the Values They Do?
Many of the fundamental constants in our universe seem precisely set in the
range that allows life to form. This is one reason why some physicists have
been turning toward the anthropic principle, because it so readily explains
this fact.
Physicists hope, however, that a theory of everything would explain the
precision of these values — in essence, explain the reason why life itself is
allowed to exist in our universe — from fundamental principles of physics.
Black Hole Information Paradox: What
Happens to Missing Black Hole Matter?
The current thinking on the black hole information paradox is that there is
a quantum system underlying the black hole, and that this quantum system
never loses information, though the system can mix up the finer points in a
complicated way. To reconcile this picture with Hawking's calculations
3U2
Part VI: The Part of Tens _
(see Chapter 14), the concept of complementarity is sometimes invoked. This
idea, proposed by Leonard Susskind, says that someone outside the black
hole may observe different results than someone falling into the black hole,
but that no contradictions will arise.
This approach hasn't settled the problem for everyone, including physicists
who believe that relativity should hold more sway than quantum mechanics.
Whatever the solution, a theory of everything would have to present a
definitive set of rules that could be applied to figure out what's happening to
matter (and information) that falls into a black hole.
Quantum Interpretation: What Does
Quantum Mechanics Mean)
Though quantum mechanics works to explain the results seen in laboratory
experiments, there's still not a single clear description of the physical
principle that causes it to work the way it does. Though this is tied to the
"collapse of the quantum wavefunction," the exact physical meaning of the
wavefunction, or of its collapse, remains a bit of a mystery. (So if you don't
understand quantum physics, don't worry . . . physicists are still debating it,
even after all these years.)
In Chapter 7, 1 explain some of the interpretations of what this may mean —
the Copenhagen interpretation, the many worlds interpretation (MWI),
consistent histories, and so on — but the fact is that these are just guesses,
and physicists really don't know for sure what's going on with this strange
quantum behavior. Lee Smolin listed this as his second "great problem in
theoretical physics." Though today this is by far the minority opinion among
physicists, the great physicists of the quantum revolution — Bohr, Einstein,
Heisenberg, Schroedinger, and the rest — also saw it as a key question to
resolve.
Today, most physicists tend to just trust in the math and don't worry about
strange things happening behind the scenes. They are perfectly comfortable
with quantum mechanics, seeing nothing mysterious in the behavior. (After
all, they have equations that describe it!)
In fact, the majority of theoretical physicists don't seem to believe that it's
possible to determine one interpretation as correct, and don't even consider
it as a question that needs to be answered, even by a theory of everything.
Some of those who do want a clear interpretation hope that a theory of
everything will provide insights into the physical mechanism explaining
quantum phenomena.
Chapter 20: Ten Questions a Theory of Everything Should (Ideally) Answer J*}3
Bark Mystery Mo. 1: What 1$ Dark
Matter (and Why 1$ There So Much)}
There appear to be two forms of matter in the universe: visible matter and
dark matter. Scientists know dark matter exists because they can detect its
gravitational effects, but they can't currently observe dark matter directly. If
extra matter weren't there to hold galaxies together, the equations of general
relativity show that they would fly apart.
Still, no one knows what the dark matter is made of. Some theorize that the
dark matter may be stable superpartners of our known particles — perhaps
photinos, the superpartner of the photon. String theory contains other ideas,
covered in Chapter 14, that could explain the nature of dark matter.
But the fact is that no one knows for sure, which is disturbing because there
is about five times as much dark matter as there is visible matter in the
universe. So there should be a lot of it around to study — if only physicists
and their scientific theories could see it for what it really is.
bark Mystery No. 2: What 1$ Dark
Energy (and Why 1$ It So Weak)}
There's a lot of dark energy in the universe — about three times as much as
visible matter and dark matter put together! This energy represents a repulsive
force of gravity on large scales, pushing the edges of the universe apart.
The abundance of dark energy by itself isn't so much a problem; the real
problem is that the dark energy is a lot weaker than physicists would
expect from purely theoretical calculations based on quantum field theory.
According to those calculations, the random energy of empty space (the
"vacuum energy") should explode up to huge quantities, but instead it
maintains an incredibly small value.
A theory of everything would hopefully explain why the vacuum energy
contains the value it does.
31*1*
Part VI: The Part of Tens _
Time Symmetry: Why Does Time
Seem to Mo</e Forward}
The space dimensions are interchangeable, but time is distinct because it
seems to move in only one direction. This doesn't have to be the case. In fact,
the mathematical laws of physics work either way, even in a universe where
time could run backwards.
But time doesn't run backwards at all, and a theory of everything would need
to explain this discrepancy between the mathematical symmetry of time and
the physical asymmetry of time that you observe every time you're running
late for a meeting.
The End of the Universe:
What Comes Next}
And, of course, the eternal question of the fate of the universe is another
question that a theory of everything would need to answer. (Cue up the song
"It's the End of the World as We Know It" by R.E.M.) Will our universe (and
all the others) end in ice, expanding until heat dissipates out across the
vastness of space? Will galaxies huddle together in dense clusters, like winter
campers around a campfire? Will the universe contract together and perhaps
eventually start the cycle of universal creation all over?
Chances are that these questions will be answered long after we're gone, but
there is hope that the beginnings of those answers may come within the
next few years, as some aspects of string theory begin to enter the realm of
experimental verification.
Chapter 21
Ten Notable String Theorists
In This Chapter
Meeting the founders of string theory
Rising to the challenge: A new generation of string theorists
Branching out to make string theory popular among nonphysicists
J\]o new theory can develop without dedicated scientists working hard
/ Wto refine and interpret it. Throughout this book, you read about some
of the pioneering work in string theory. Now it's time to find out more about
some of the scientists themselves, the people who make string theory tick as
they research the mysteries of the universe within the context of this budding
science. As string theory unfolds, some of these individuals may become
legends on the order of Einstein and Newton, or they may end up finding
useful ways of presenting this complex theory in ways that the general public
can understand.
In this chapter, I introduce ten physicists who are responsible for the rise
of string theory. I give brief biographies of not only the founders of string
theory, but also some of the visionaries who have refined the theory over the
years. Some of these personalities are also physicists who have written
popular books or been involved with educational programs on the topic,
helping to broaden the general public's understanding of string theory.
However, this chapter isn't a "top ten" list, and just because a name hasn't
been included should not be taken to mean that the person's work and
contributions are any less significant than the names listed.
Edward Witten
Seen by many as the leading thinker of string theory, Witten introduced the
concept of M-theory in 1995 as a way to consolidate the existing string
theories into one comprehensive theory. Witten's work in string theory
also included the 1984 application of Calabi-Yau manifolds to explain the
compactification of the extra dimensions.
366
Part VI: The Part of Tens _
In 1951, Witten was born into physics, in a sense; his father, Louis Witten,
was a theoretical physicist specializing in general relativity. Growing up,
Witten displayed a natural aptitude for mathematics. Despite this, he focused
his early years on studying history and being politically active, helping with
George McGovern's 1972 presidential campaign. His undergraduate degree
from Brandeis University was in history with a minor in linguistics.
In the fall of 1973, Witten went to graduate school in applied mathematics
at Princeton University. Despite lacking a physics undergraduate degree, he
quickly showed himself to be proficient at the complex mathematics involved
in theoretical physics. He switched to the physics department and received
his PhD from Princeton in 1976.
Witten has since published more than 300 research papers. According to
some sources, he has the largest h-index (most often cited papers) of any
living physicist. He received the MacArthur Foundation "genius grant"
fellowship in 1982. In 1990, he was the first (and so far only) physicist to
receive the Fields Medal, sometimes informally called the "Nobel Prize of
mathematics" (the Nobel Committee awards no mathematics prize). He was
one of Time magazine's 100 most influential people in 2004.
Among string theorists, Edward Witten is seen as a guiding light because
of his ability to grasp the implications of the complex mathematics of the
theory on a level that few others have been able to match. Even the strongest
string theory critics speak of his intellect and mathematical prowess in awe,
making clear that he is an unparalleled mind of his generation.
John Henri} Schu/arz
If string theory were a religion, then John Henry Schwarz would be the
equivalent of St. Paul. At a time when virtually every other physicist
abandoned string theory, Schwarz persevered for almost a decade as one of
the few who tried to work out the theory's mathematical details, even though
it hurt his career. Eventually, his work led to the first superstring revolution.
Schwarz was one of the physicists who discovered that supersymmetry
resolved several of the problems with string theory. Later, Schwarz proposed
the idea that the spin-2 particle described by string theory may be the
graviton, meaning that string theory could be the long-sought theory to unify
quantum physics and general relativity. (See Chapter 10 for more on these
concepts.)
.Chapter 21: Ten Notable String Theorists 3^ 7
Schwarz worked at Caltech for 12 years — from 1972 to 1984 — as a temporary
researcher instead of a full professor. His career prospects were hindered in
large part because of his perceived obsession with string theory.
In 1984, Schwarz performed (along with Michael Green) the work showing
that string theory was consistent, triggering the first superstring revolution.
Without Schwarz's decade of dedicated work (or obsession), there would
have been no foundation in place for superstring theory to build upon
throughout the 1980s, when it rose to prominence among particle physicists.
l/oichiro Nambu
Yoichiro Nambu is one of the founders of string theory who independently
discovered the physical description of the Veneziano model as vibrating
strings. Nambu was already a respected particle physicist for his earlier work
in describing the mechanism of spontaneous symmetry breaking in particle
physics. Dr. Nambu received the 2008 Nobel Prize in Physics for this work.
Though this makes him the only founder of string theory to have received a
Nobel Prize, it's important to note that the Nobel award makes no mention
of string theory. In fact, the Nobel can't be awarded for theoretical work that
hasn't been confirmed or proved useful experimentally.
Leonard Susskind
Leonard Susskind is another founder of string theory. As he recounts in
his book The Cosmic Landscape: String Theory and the Illusion of Intelligent
Design, he saw the original dual resonance model equations and thought they
looked similar to equations for oscillators, which led him to create the string
description — concurrently with Yoichiro Nambu and Holger Nielson. In
addition, he has proposed several concepts discussed throughout this
book: string theory of black hole entropy (Chapter 14), the holographic
principle (Chapter 11), matrix theory (Chapter 11), and the application of the
anthropic principle to the string theory landscape (which is the subject of
The Cosmic Landscape; I cover this principle in Chapter 11).
In addition to his extensive work in string theory, Susskind is well-known for
his disagreements with Stephen Hawking over the final fate of information that
falls into a black hole, as outlined in his 2008 book The Black Hole War: My
Battle with Stephen Hawking to Make the World Safe for Quantum Mechanics.
31*8
Part VI: The Part of Tens _
tUulid Grass
David Gross was one of the physicists who developed the heterotic string
theory, one of the major findings of the first superstring revolution.
In 2004, Gross earned (along with colleagues Frank Wilczek and David
Politzer) the Nobel Prize in Physics for their 1973 discovery of asymptotic
freedom in the strong nuclear interaction of quarks. (This means that the
strong interaction between quarks gets weaker at extremely short distances.)
Since 1997, Dr. Gross has been the director of the Kavli Institute for
Theoretical Physics at the University of California, Santa Barbara. In this
capacity, Gross is known not only as a strong advocate for string theory but
also as a strong opponent of the anthropic principle as applied to the string
theory landscape.
Joe Polchinski
Joe Polchinski proved that string theory required objects of more than one
dimension, called branes. Although the concept of branes had previously
been introduced, Polchinski explored the nature of D-branes. This work was
crucial to the second superstring revolution of 1995. Polchinski's work is
seen as fundamental to the development of M-theory, brane world scenarios,
and the holographic principle (all covered in Chapter 11).
Lately, Polchinski has become a convert to the anthropic principle's
usefulness in string theory, though stories abound of how he once loathed
the principle, considering it unscientific and threatening to quit his position
if he were forced to adopt it.
Juan Maldacena
Juan Maldacena is an Argentine physicist who developed the idea that a
duality exists between string theory and a quantum field theory — called the
Malcadena duality (or the AdS/CFT correspondence; see Chapter 11).
The Maldacena duality, proposed in 1997, has been applied only in certain
cases, but if it can be extended to all of string theory, it would allow a means
to give a precise quantum string theory. In other words, string theorists
.Chapter 21: Ten Notable String Theorists 3^ y
should be able to translate known principles of gauge field theory into string
theory equations — an excellent starting point for a complete quantum
theory of gravity. Also, applying the duality in the other direction, starting
with string theory and creating predictions about how gauge theory should
behave could yield predictions that are testable at the Relativistic Heavy Ion
Collider or Large Hadron Collider in years to come.
Lisa Randaii
Theoretical physics is a realm stereotypically dominated by men and, even
among the rare women who choose it, Lisa Randall doesn't fit the mold.
She spends her free time on intense rock climbing expeditions but spends
her professional days exploring the implications of multidimensional brane
worlds as a phenomenologist.
Dr. Randall was the first tenured woman in the physics department at
Princeton University. She was also the first tenured female theoretical
physicist at MIT and later at Harvard, where she has been since 2001.
Randall rose to prominence among nonphysicists with her 2005 book Warped
Passages: Unraveling the Mysteries of the Universe's Hidden Dimensions.
Among other things, this resulted in her appearance on Comedy Central's
wildly popular mock political pundit show, The Colbert Report.
Given her success as a woman in a male-dominated field, it's not surprising
that she has impressive credentials. One of the most intriguing models to
come out of her analysis of brane world scenarios are the Randall-Sundrum
models, which explore the possibility of gravity behaving differently off of
our own 3-brane.
Michio Kaku
Physicist Michio Kaku has been one of the most vocal supporters of string
theory. He worked on the theory early in the 1970s, actually co-founding
"string field theory" by writing string theory in a field form. By his own
account, he then abandoned work on string theory because he didn't believe
in the additional dimensions the theory demanded. He returned to string
theory during the first superstring revolution and has proven an entertaining
and lucid spokesman ever since.
350
Part VI: The Part of Tens _
Dr. Kaku wrote one of the first popular books on the topic, Hyperspace:
A Scientific Odyssey Through Parallel Universes, Time Warps, and the 10th
Dimension, in 1994. (This was my first introduction to string theory, when I
read the book as a high school senior.) He has since written other books on
futurism and advanced scientific and technology principles. His 2005 book,
Parallel Worlds, focuses on many topics related to string theory.
For more than 25 years, Kaku has been a professor of theoretical physics at
the City College of New York. The close proximity to major television networks
may explain why he regularly appears on so many television programs. With
a distinctive mane of white hair, Dr. Kaku is easily recognizable when he
makes appearances on CNN, Discovery, the Science Channel, or ABC's Good
Morning, America. (When GMA needed someone to explain how Mentos cause
soda bottles to erupt into fountains of fizz, they called in Dr. Kaku.)
Kaku has also hosted a number of programs, including two of his own radio
shows. He is currently seen hosting the SciQ Sunday specials on the Science
Channel. His research work on the subject of string theory isn't as impressive
as the others on this list, but he has done an incredible amount to popularize
the ideas of string theory. Many recognize him as one of the theory's most
vocal proponents to layman audiences.
Brian Greene
Last but certainly not least is probably one of the best-known string theorists,
especially among nonphysicists. Brian Greene's popularity as a writer and
spokesman for the field dates back to his 1999 book The Elegant Universe:
Superstrings, Hidden Dimensions, and the Quest for the Ultimate Theory, which
was used in 2003 as the basis for a three-part PBS Nova special. In 2004,
Greene followed up with the book The Fabric of the Cosmos: Space, Time,
and the Fabric of Reality. (He has appeared on Comedy Central's The Colbert
Report at least twice, outdoing Dr. Randall's one appearance.)
Dr. Greene earned his undergraduate degree from Harvard. As a Rhodes
Scholar, he received a 1986 doctorate from Oxford University. He was a
professor at Cornell University for several years, but has been a full professor
at Columbia University since 1996. Throughout his career, his research has
focused on quantum geometry and attempting to understand the physical
meaning of the extra dimensions implied by string theory.
In addition to trying to explain string theory to the masses, Greene has been
co-director of Columbia University's Institute for Strings, Cosmology and
Astroparticle Physics (ISCAP) since its founding in 2000.
In 2008, Greene was a founder of the World Science Festival in New York City,
where a dance troupe performed an interpretative dance version of his book
The Elegant Universe.
Index
• Numerics •
l-dimensional objects, 12
1-dimensional waves, 169
2-dimensional brane
(2-brane), 13-14
2-dimensional space
Cartesian geometry,
231-233
Euclidean geometry, 231
3-dimensional space
Mobius strip, 234-236
non-Euclidean geometry,
236-237
Vectors, 233-234
4-dimensional string
theories, 241-243, 255
4-simplices, 324-325
1 1-dimensional supergravity
theory, 176, 188-189
•A*
Abbott, Edwin A., 232
accelerating expansion of
universe, 44-45
acceleration, in laws of
motion, 73-74
acceleration rates, and
mass, 27
accelerators, particle. See
particle accelerators
AdS/CFT (anti-de Sitter/
conformal field theory)
correspondence, 41,
199-200, 348
aether, 65, 138
Akeno Giant Air Shower
Array (AGASA)
project, 221
Akulov, Vladimir, 171
Albrecht, Aldreas, 330-331
Alexander, Stephon, 216
Alpher, Ralph, 148
alternate history, 268
Amelino-Camelia, Giovanni,
219-220
amplitude, 69
analogy, 239
analytic geometry, 231
Anderson, Poul, 293
anode, 122
anomalies, string theory,
177-178
Anthropic Cosmological
Principle, The
(book), 114
anthropic principle
controversy about, 19
dark energy, 256
fine-tuning of universe,
259-260
observers, need of in,
204-206
PAP, 114
string theory controversy,
303-305
value of, 207-208
anti-de Sitter space, 144, 200
anti-de Sitter/conformal
field theory (AdS/CFT)
correspondence, 41,
199-200, 348
antigravity, 144
antimatter, 127-128
antinodes, 71-72
anti-strings, 248
appeal to authority, 307
approximation method, 187
argumentum ad
verecundiam, 307
Aristotle, 138-139
Aristotle and an Aardvark
go to Washington:
Understanding Political
Doublespeak Through
Philosophy and
Jokes (book), 304
Arkani-Hamed, Nima, 202
arrow of time, 276-278
artwork, 237
Ashtekar, Abhay, 315
astrologer, 140
astronomer, 140
astrophysicist, 140
astrophysics. See cosmology
and astrophysics
asymmetry, 60, 277
asymptotic freedom, 325
asymptotic safety, 324-326
atom, 29-30. See also
atomic theory
atomic theory
electrons, 122-123
movement within atom,
123-125
nuclei, 123
overview, 120-121
attractive gravity, 154
Augustine of Alexandria,
St., 278
authority, appeal to, 307
axion, 222, 289
•B
Back to the Future (film), 293
background-dependent
theory, 97, 310, 314-315
background-independent
theory, 309
Baconian model, 53
Barrett-Crane model, 319
Barrow, John, 114
Bars, Itzhak, 288-289
baryon asymmetry, 340
baryonic matter, 153, 340
basis, vector space, 234
Bekenstein, Jacob, 157
bending dimensions, 239-240
Bernoulli, David, 120
big bang theory
chemical elements, origin
of, 150
cosmic microwave
background radiation,
148-149
overview, 21, 340
steady state theory,
147-148
jf}2 String Theory For Dummies _
Big Bang Theory, The
(sitcom), 321
big bounce, 258
big crunch, 257-258
big freeze, 257
big splat theory, 249
Bilson-Thompson, Sundance
0..316
black holes
branes, explaining with,
194-195
conditions at edge of,
157-158
conditions inside, 156-157
event horizons, 282
extremal, 195, 251
information paradox, 157,
252-253, 272, 341-342
loop quantum gravity,
317-318
overview, 95-96
string theory explanation
of, 40-41,250-253
thermodynamics, 250-252
blackbody, 80, 100-102
Blanqui, Louis Auguste, 263
Bohm, David, 116
Born, Max, 111
bosonic string theory
dimensions, space and
time, 168-170
electrons, absence of
in, 168
massless particles, 166-167
overview, 161-162
particles, 162-165
versus Standard Model,
165-166
tachyons, 167-168
bosons. See also bosonic
string theory
with fermions in
superstring theory,
171-172
gauge, 36, 133-134
Higgs, 134-135
overview, 131-132
supersymmetry, 15, 37, 211
bottle, Klein, 235-236
Brahe, Tycho, 142
Brandenberger, Robert,
247-248
brane smash theory, 249
brane worlds, 195-196
branes
black holes, 194-195,
251-252
brane worlds, 195-196
D-branes, 190-191
M-theory, 11, 183
overview, 3, 12-14
p-branes, creating particles
from, 192
required by M-theory,
192-193
uniting D-branes and
p-branes, 193-194
wormholes, 272
bridge, Einstein-Rosen, 20,
284-285
broken symmetry, 60-62,
68,213
Brownian motion, 121
Bruno, Giordano, 263
bubble u
bulk, 190
•C»
Calabi-Yau manifolds, 163,
180-182
calculus, 75
Carroll, Lewis, 232
Carter, Brandon, 205
Cartesian geometry, 231-233
cat experiment,
Schrodinger's, 111-112
Cathcart, Thomas, 304
cathode, 122
cathode ray tube, 122
causal dynamical
triangulations (CDT),
324-325
censorship conjecture,
cosmic, 280
chaotic inflation, 265-266
charge
color, 131
D-brane, 193
dimensions, 241-242
electrical, 77
charge-conjugation
symmetry, 68, 277
charge-conjugation/parity
(CPT) symmetry, 277
chemical elements, origin
of, 150
child universe, 274
Chinese theory of matter,
64-65
chromodynamics, quantum
nucleons, 129-130
overview, 129
quarks, 130-131
twistor theory, 334
chronology protection
conjecture, 279-280
classical physics
acceleration, 73-74
calculus, 75
electricity, 77
electromagnetic waves, 79
ether theory, 76-79
Faraday force field
proposal, 78-79
force, 73-74
gravity, 74
kinetic energy, 66
light, as waves, 76-79
magnetism, 77
mass, 73-74
mathematics, 75
matter, 64-65
Maxwell's equations, 79
modern physics, birth of, 80
motion, 73-74
optics, 75
overview, 63-68
potential energy, 66-67
symmetry, 67-68
vibrations, 70-72
waves, 69-70
classical view of matter, 29
CLIC (Compact Linear
Collider), 226
closed strings, 12-14, 175
closed timelike curve, 282
closed u
CMBR (cc
background radiation),
148-149, 151, 214-215,
221,327
cold death, 257
color charge, 130
Compact Linear Collider
(CLIC), 226
Jndex 353
compactification
Calabi-Yau manifolds, 180
dimensions, 16, 214
methods of, 239-240
overview, 10
composite bosons, 132
composite fermions, 133
computer, quantum, 333
Confessions (book), 278
configuration, extremal, 195
confirmation, of theories,
54-55
conformal symmetry, 169
Connes, Alain, 334-335
conservation of mass, 29,
64-65
conservation of
mass-energy, 88
consistent histories view, 115
constants
cosmological, 143-144,
153-154, 200-201
coupling, 186
fine-structure, 331
values of fundamental, 341
contraction of universe, 22
controversy, string theory
outlining arguments,
298-301
overview, 297
rebuttal, 311-312
scientific theory, success
as, 301-305
string theorists, criticism
of, 305-308
universe, description of,
308-311
conventions used in book,
2-3
convergence, 187
Conversations on the Plurality
of Worlds (book), 263
Copenhagen
interpretation, 113
Copernican principle,
141-142
Copernicus, Nicholas,
141-142
cosmic censorship
conjecture, 280
Cosmic Landscape, The
(book), 196
cosmic microwave
background radiation
(CMBR), 148-149, 151,
214-215, 221, 327
cosmic rays, 218, 220-222
cosmic strings, crossing
to allow time travel,
286-287
cosmic superstrings,
detecting, 222-223
cosmic topology, 240
cosmological constant,
143-144, 153-154,
200-201
cosmological principle, 143
cosmologist, 140
cosmology and astrophysics
big bang theory, 147-150
black holes, 156-158
dark energy, 153-155
dark matter, 153
expansion of universe,
143-146
heliocentric view, 141-142
incorrect models of
universe, 138-140
inflation theory, 151-152
overview, 21,95-96, 137
cosmos, future of, 257-258
Coulomb's Law, 77
coupling constant, 186
covariance, principle of, 91
CP violations, 277
CPT (charge-conjugation/
parity) symmetry, 277
Cremmer, Eugene, 176
crest, 69-70
•/>•
Dai, Jin, 190-191
Dalton, John, 120
dark energy
analyzing, 222
cosmological constant,
143-144
not predicted by string
theory, 44-45
overview, 153-155, 200-201,
255-256
weakness of, 343
dark matter
analyzing, 222
MOND, 328-330
mystery surrounding, 343
overview, 153, 255
D-branes, 190-191, 193-194
de Broglie hypothesis,
106-108
de Broglie, Louis, 116
de Sitter space, 144
de Sitter, Willem, 144
decay
proton, 304
radioactive, 32
decoherence, 113, 115
deformed special relativity
(DSR), 328
degree of freedom, 230
Democritus, 120
Descartes, Rene, 231
detector, GEO600 gravity
wave, 215
diagrams, Feynman,
125-126, 128
Dicke, Robert, 148-149
dilation, time, 87, 157, 280
dilation field, 186
dimensions
2-dimensional space,
230-233
3-dimensional space,
233-237
adding, 238-239
bending, 239-240
denning, 229-230
extra, 15-16, 241-243, 309
Kaluza-Klein theory, 96-97
overview, 229-230
spacelike, 237
space-time, four dimensions
of, 237-238
space-time continuum, 85
testing for, 210
time, 287-289
timelike, 237
torus, 16-17
uncurling of, proposals
for, 201
Dimopoulos, Savas, 202
"Direct Empirical Proof of the
Existence of Dark Matter,
A" (paper), 330
jjll String Theory For Dummies _
Dirichlet boundary
condition, 191
discrete energy packets, 102
disproving string theory,
215-216
Doppler effect, 146
double slit experiment,
105-111
doubly special relativity
(DSR), 328
dragging, frame, 283
Dreyer, Olaf, 327
DSR (deformed special
relativity), 328
DSR (doubly special
relativity), 328
dual problem, 251
dual resonance models, 162,
165-166
dualities
overview, 184
strong-weak, 186-187
topological, 185-186
using two to unite five
superstring theories,
188-189
Dvali, Gia, 202
•£•
E=mc 2 equation, 22-23, 87-88
earth, as center of universe,
139-140
Eddington, Arthur, 276-277
effective theory, 298
Einstein, Albert
applying work to mysteries
of universe, 95-96
atomic theory, 121
black hole event
horizons, 282
cosmological constant,
143-144
curvature of light, 94-95
general relativity theory,
development of, 60
law of gravity, 28
light, 102-104
objectivity, 56
Planck scale breakdown of
general relativity, 220
simplicity, 56
singularities, 33
space-time theory, 18, 60
special relativity, 60, 281
time travel through
wormholes, 284-285
Einstein-Rosen bridge, 20,
284-285
ekpyrotic universe theory,
21, 247-250, 256, 266
electric current, 31, 77
electric flux, 201
electrical charge, 77
electricity
developments using, 23
relationship to magnetism,
31,77
electrodynamics, quantum
antimatter, 127-128
overview, 31, 125
particle information
exchange, 125-127
virtual particles, 128-129
electromagnetic force, 14, 18
electromagnetic waves, 79
electromagnetism, 30-31,
59,76
electrons
bosonic string theory, 168
de Broglie hypothesis,
106-107
overview, 31, 122-123
photoelectric effect,
103-104
electrostatics, 77
electroweak force, 134
elements, 120
Elements book, 231
11-dimensional supergravity
theory, 176, 188-189
end of universe, 22, 344
energy. See also dark energy
hierarchy issues, 341
kinetic, 66
negative, 286
Planck, 117-118
potential, 66-67
unifying with mass, 87-88
vacuum, 136, 343
energy hill, 265
energy packets, discrete, 102
entropy
arrow of time, 277
big freeze model, 257
black holes, 157
cyclic universe model, 247
extremal black holes, 251
loop quantum gravity, 317
equations
E=mc 2 , 22-23, 87-88
electromagnetic wave, 79
F=ma, 73
field, 91
Schrodinger, 267
equivalence, principle of,
89-90
eternal inflation, 253-254,
264-266
eternal universe model, 246,
318
Eternity by the Stars:
Astronomical Hypotheses
(brochure), 263
ether
searching for, 82-83
theory of, 76-79
Euclidean geometry, 231
Euler beta function, 163
event horizon, black hole,
157, 282
Everett, Hugh, III, 114,267
evolution, of universe,
253-256
exclusion principle,
Pauli, 132
expansion of universe
gravity, in energy and
pressure, 143-145
Hubble's discovery of,
145-146
overview, 143
experimental complications,
of string theory, 46-47
experimental evidence,
46-47, 52
experimental falsifiability,
53-55
exploring universe
cosmic superstrings,
detecting, 222-223
dark energy, analyzing, 222
dark matter, analyzing, 222
outer space rays, using to
amplify small events,
219-222
219
355
extra-dimensional gravity,
testing
gravity waves in CMBR,
searching for, 214-215
inverse square law, 214
overview, 213
extremal black hole, 195, 251
extremal configuration, 195
•F»
F=ma equatic
false vacuum, 265
falsifiability, 53-55, 302
Faraday, Michael, 76-79
Feinberg, Gerald, 290
Feinberg reinterpretation
principle, 290
Fermi Gamma-ray Space
Telescope, 220
fermions
in string theory, 168
in superstring theory,
171-172
supersymmetry, 15, 37, 211
Ferrara, Sergio, 176
Feynman diagrams, 125-126,
128, 278-279
fiction, science, 293
field equations, 91
field theory, 11,34
fields
dilation, 186
Higgs, 134-135
inflaton, 152
loop quantum gravity, 314
overview, 11
phion, 332
fine-structure constant, 331
finite theorem, loop quantum
gravity, 318-319
finiteness of string theory,
310-311
first law of motion, 74
flat universe, 145
Flatland: A Romance of Many
Dimensions (book), 232
flatness problem, inflation
theory, 151-152
flavor problem, 213
flavors, of quarks, 130
Fly's Eye cosmic ray
observatory, 221
foam, quantum, 33-34,
117,129
Fontenelle, Bernard le Bovier
de, 263
defined, 64
in laws of motion, 73-74
force fields, 78-79
forces
electromagnetism, 30-31,
59,76
hierarchy issues, 341
nuclear, 31-32
unification of, 14, 18
4-dimensional string
theories, 241-243, 255
4-simplices, 324-325
frame dragging, 283
Freedman, Daniel, 176
freedom
asymptotic, 325
degree of, 230
frequency, 70-71, 103-104
Frequency (film), 293
Friedmann, Aleksandr,
144-146
F-theory, 203
fundamental constants,
values of, 341
fundamental frequency, 71
fundamental theories, 45, 298
future complications of
string theory, 46-47
future of cosmos, 257-258
Galileo Galilei, 142
gamma ray bursts (GRBs),
218-220, 318
Gamow, George, 148-150
Gates, S. James, Jr., 241-242
Gateway (novel), 293
gauge bosons, 36, 131,
133-134
gauge theory, 36, 134-135
Gauss, Carl Friedrich, 236
Geiger, Hans, 123
Gell-Mann, Murray, 130
general relativity
background-independency,
309-310
black hole event
horizons, 282
cosmological constant,
143-144
curvature of light, 94-95
development of, 28, 60
gravity as acceleration,
89-90
gravity as geometry, 91-92
Planck scale breakdown
of, 220
quantum physics, 32
singularities, 33
theory of gravity,
competition for, 93
wormholes, 282-286
GEO600 gravity wave
detector, 215
geodesic, 28
geometric symmetry, 67
geometry
Cartesian, 231-233
Euclidean, 231
non-Euclidean, 236-237
Georgi-Glashow model, 217
geosynchronous model, 139
Glashow, Sheldon Lee, 134
global positioning system
(GPS), 92
gluon,31, 130-131
Godel, Kurt, 283
Golfand, Yuri, 171
Gott, J. Richard, 287
GPS (global positioning
system), 92
grand unification theories
(GUTs), 217-218
grandfather paradox, 292
graphity, quantum, 324,
326-327
gravitational constant, 74
gravitational field, 78
gravitational lensing, 223, 330
gravitons, 14, 36, 40, 132, 134,
167, 174-175
330 String Theory For Dummies _
gravity. See also laws of
gravity; loop quantum
gravity; quantum gravity
11-dimensional
supergravity theory, 176,
188-189
as acceleration, 89-90
antigravity, 144
attractive, 154
black holes, 156-157
competition for theory
of, 93
dark energy, 154
in energy and pressure,
143-145
extra-dimensional, testing,
213-215
as geometry, 91-92
localized, 203
locally localized, 203-204
metric theory of, 93
Metric-Skew-Tensor
Gravity, 332
overview, 74
predicting out of strings, 40
Randall-Sundrum models,
202-203
repulsive, 154
Scalar-Tensor-Vector
Gravity, 332
testing inverse square
law, 214
unified theory of forces,
14, 18
gravity wave detector,
GEO600, 215
gravitybrane, 203
GRBs (gamma ray bursts),
218-220, 318
Greek theory of matter,
64-65, 120, 138
Greene, Brian, 307, 350
greybody factors, 251
Gross, David, 348
ground state, 67
group representation
theory, 216
Guendelman, Eduardo, 274
Guth, Alan, 152
GUTs (grand unification
theories), 217-218
GZK cutoff energy, 221
• H*
hadrons, 11, 130
Hafele-Keating
experiments, 281
harmonic oscillators, 68
harmonics, 72
Hawking, Stephen
black hole thermodynamics
argument, 251-253
chronology protection
conjecture, 279-280
Hawking radiation, 157
Perimeter Institute, 327
Hawking radiation, 157-158,
250,317
heavenly bodies, movements
of, 142
Heisenberg, Werner, 108-109
heliocentric view, 141-142
Herman, Robert, 148
heterotic string theory,
179-180, 242
hidden variables
interpretation, 115-116
hierarchy issues,
135-136, 341
Higgs, Peter, 135
Higgs boson, 134-135
Higgs field, 134-135
Higgs mechanism, 134-135
high-energy physics, 56
Hilbert space, 267-268
h-index, 306, 346
Hindu cosmology, 262
Hogan, Craig, 215
hologram
denned, 199
universe as, 21
holographic principle
AdS/CFT correspondence,
199-200
connecting to reality,
198-199
denned, 21
detecting with gravity
waves, 215
multidimensional
information, capturing
on flat surface, 197-198
homogeneity problem,
151-152
Hooft, Gerard 't, 197-198
horizon problem, 152, 326,
329-330
Hoyle, Fred, 147-148, 150
Hubble, Edwin, 143, 145-146
Hubble volume, 264
Huxley, Thomas Henry, 54
hypercube, 239
hyperspace, history of
extra dimensions, location
of, 270-271
wormholes, 271-272
• ;
icons used in book, 6
ILC (International Linear
Collider), 226
imaginary number, 167
indestructibility of mass, 65
inductive logic, 52
inductive reasoning, 53
inertial frames of
reference, 84
infinite dimensions, 202-204
infinities
blackbodies, 101
QED, 127
quantum jitters, 33-34
renormalization, 136
singularities, 33
string theory, 177
inflation
chaotic, 265-266
eternal, 253-254, 264-266
inflation theory
flatness problem, 151
horizon problem, 151
overview, 21
rapid expansion, 152
inflaton, 152
inflaton field, 152
information exchange,
particle, 125-127
information paradox, black
hole, 157, 252-253, 272,
341-342
information theory,
quantum, 333
interference, 70, 106-108, 110
interferometer, 82-83
internal relativity, 324, 327
internal symmetry, 67-68
Jndex 357
International Linear Collider
(ILC), 226
interpretation, quantum, 342
inverse square law of
gravity, 214
island universes, 254
isotopic charge space, 241
James, William, 262
jitters, quantum, 33-34
Julia, Bernard, 176
Just Six Numbers: The Deep
Forces That Shape the
Universe (book), 258-259
K
Kaku, Michio, 174, 349-350
Kaluza-Klein theory, 35,
96-98
Karch, Andreas, 203
Kemmer, Nicolas, 241
Kepler, Johannes, 142
Kerr, Roy, 285
Kerr black hole, 285
kinematics, 26
kinetic energy, 66
Klein, Daniel, 304
Klein bottle, 235-236
Kuhn's model, 58
• £•
Large Hadron Collider (LHC),
224-226
Lavoisier, Antoine-Laurent, 65
law of universal gravitation, 74
laws of gravity
doubly special
relativity, 328
gravity as force, 26-28
gravity as geometry, 28
inverse square, 214
modified gravity, 216,
330-332
modified Newtonian
dynamics, 328-329
variable speed of light, 216,
329-331
laws of motion, 73-74
laws of physics, 60-61
Lazaridis, Mike, 327
Leibniz, Gottfried, 75
Leigh, Rob, 190-191
LemaTtre, Georges, 146-147
length, Planck, 117-118, 328
lensing, gravitational,
223, 330
leptons, 132-133
Level 1 parallel u
262, 264-265
Level 2 parallel u
262, 265-267
Level 3 parallel universes,
262, 267-268
Level 4 parallel universes,
263, 269-270
LHC (Large Hadron Collider),
224-226
light
following bouncing beam
of, 85-87
speed of, 84-86, 330
theory of, 311
as waves, 76-79
Likhtman, Evgeny, 171
Linde, Andrei, 214,254,265
linear algebra, 234
linear symmetry, 60
Lloyd, Seth, 333
localized gravity, 203
locally localized gravity,
203-204
Logic of Scientific Discovery,
The (book), 54
Loll, Renate, 325
longitudinal wave, 69, 169
loop quantum gravity
background-dependence,
314-315
big bounce, 258
finite theorem, benefit of,
318-319
flaws, 319-320
looping, defining, 314-316
overview, 18, 313
predictions, 317-318
space-time, 279
versus string theory,
320-321
Lorentz invariance, 330
Lovelace, Claude, 168
Luminet, Jean-Pierre, 240
luminous ether, 76
• M*
magnetism, 31, 77
Magueijo, Joao, 216, 330-331
Maldacena, Juan, 199-200,
252, 348-349
Maldacena conjecture,
41,224
Maldacena duality, 348
Mandelstam, Stanley, 310
Many Worlds in One:
The Search for Other
Universes (book), 265
many worlds interpretation
(MWI), 114-115,
267-268, 292
Markopoulou, Fotini, 326, 333
Marsden, Ernest, 123
mass
conservation of, 29, 64-65
explaining, 16-17
Higgs mechanism, 134-135
indestructibility of, 65
Newton's gravitational
theory, 26-27
overview, 64-65, 73-74
Planck, 117
unifying with energy, 87-88
mass-energy, conservation
of, 88
massless particles, 166-167
mathematical democracy
principle, 269
mathematical
inconsistencies, string
theory, 216
Mathematical Principles of
Natural Philosophy
(book), 73
mathematics
applications of, 163
foundation of theory, 55-56
overview, 75
jjO String Theory For Dummies _
Matrix theory, as potential
M-Theory, 196-197
matter
baryonic, 153, 340
classical view, 29
dark, 153, 222, 255,
328-330, 343
early understanding of,
64-65
explaining, 16-17
indestructibility of mass, 6;
quantum scale view, 29-30
Maxwell, James Clerk, 31, 79
MDM (millimeter dimension
model), 202
mechanical waves, 68-70
mechanics
overview, 26
quantum, 272-274
temporal, 276-280
mesons, 132, 221
messages, sending through
time, 290
messenger photon, 126
metric theory of gravity, 93
Metric-Skew-Tensor Gravity
(MSTG), 332
Michelson, Albert, 82-83
Michelson-Morley
interferometer, 82-83
Milgrom, Mordehai, 329
millimeter dimension model
(MDM), 202
Minkowski, Hermann, 87,
237-238
Minkowski diagram, 87
Minkowski space, 237
Mobius strip, 234-236
modern physics, birth of, 80
modes, vibrational, 72
modified gravity (MOG)
theory, 216, 330-332
modified Newtonian
dynamics (MOND),
328-329
Moffat, John, 216, 306,
329-332
molecules, 120
Morley, Edward, 82-83
motion, laws of, 73-74
movement of heavenly
bodies, 142
MSTG (Metric-Skew-Tensor
Gravity), 332
M-theory
branes, 192-193
dualities, 184-189
Matrix theory, 196-197
overview, 3, 11-12, 46,
183-184
two-time physics, 288
multidimensional
information, capturing
on flat surface, 197-198
multiverses. See also parallel
universes
anthropic principle,
204-206
black hole information
paradox, 253-254
Level 1, 264-265
Level 2, 265-267
Level 3, 267-268
Level 4, 269-270
overview, 261-263
MWI (many worlds
interpretation), 114-115,
267-268, 292
•A/»
Nagaoka, Hantaro, 123
Nambu, Yoichiro, 165, 347
natural units, 117
nebulae, 145
negative energy, 286
negative evidence, 53
neo-darwinism, 59
neutrinos, 167, 217-218
neutrons, 32, 129-131
Neveu, Andre, 171, 173
Newton, Sir Isaac, 26-28
Newton's constant, 74
NGT (nonsymmetric
gravitational theory),
331-332
Nielsen, Holger, 165
nodes, 71-72, 315
noncommutative geometry,
334-335
non-Euclidean geometry,
236-237
non-inertial frames of
reference, 89
nonsymmetric gravitational
theory (NGT), 331-332
Nordstrom, Gunnar, 93,
96-97
normal modes, 72
nuclear forces, 31-32
nuclei, 123
nucleons, 129-130
nucleosynthesis, stellar, 150
•0*
objectivity, role in
science, 57
Occam's razor, 56-57,
242, 302
On the Revolutions of the
Celestial Spheres (book),
141-142
1-dimensional objects, 12
1-dimensional waves, 169
open strings, 12-13, 175
open universe, 145
optics, 75
oscillators, harmonic, 68
outer space rays, using to
amplify small events
cosmic rays, 220-222
gamma ray bursts, 219-220
overview, 218-219
.p.
packets, discrete energy, 102
paradigms, scientific, 58-59
parallel postulate, 236
parallel universes
hyperspace, history of,
270-272
Level 1, 262, 264-265
Level 2, 262, 265-267
Level 3, 262, 267-268
Level 4, 263, 269-270
many worlds interpretation,
114-115,267-268,292
overview, 20, 261-263
quantum mechanics in
transportation, 272-274
parity, 180
parity symmetry, 277
participatory anthropic
principle, 113-114
359
particle accelerators
colliders of future, 226
Large Hadron Collider,
224-226
overview, 130
Relativistic Heavy Ion
Collider, 224
particle information
exchange, 125-127
particle physics, Standard
Model of
atomic theory, 120-125
versus bosonic string
theory, 165-166
bosons, 132
fermions, 132-133
gauge bosons, 133-134
hierarchy problem, 135-136
overview, 119
quantum chromodynamics,
129-131
quantum electrodynamics,
125-129
spontaneous symmetry
breaking, 68
supersymmetry, 37-38
theory of where mass
comes from, exploring,
134-135
unification, 35-36, 60
particles
of atoms, 30
axion, 222, 289
bosons, 15, 36-37, 131-132,
134-135, 171-172,211
cosmic rays, 220
creation of, 221
de Broglie hypothesis,
106-108
double slit experiment,
105-106
dual resonance models, 162
electrons, 31, 103-104,
106-107, 122-123, 168
families of, 242
fermions, 15, 37, 131-133,
168,171-172,211
Feynman diagrams, 126
gluons, 31, 130-131
gravitons, 14, 36, 40, 132,
134, 167, 174-175
hadrons, 11, 130
hierarchy issues, 341
Higgs boson, 134-135
inflatons, 152
leptons, 132-133
light as, 75
massless, 166-167
mesons, 132
neutrinos, 167,217-218
neutrons, 32, 129-131
photons, 31, 85, 102-104,
126, 128, 219-220
positrons, 127
protons, 31-32, 129-131
quantum tunneling, 272-273
quantum wavefunction,
108-109
quarks, 32, 130-133, 217
scattering of, in dual
resonance models, 162
as strings, 164-165
supersymmetry, 15, 43-44
tachyons, 167-168, 290
torus, 16-17
uncertainty principle, 110
virtual, 34, 128-129
W- bosons, 31
W + bosons, 31
Z bosons, 31
partons, 44, 196-197
Pauli exclusion principle, 132
p-branes, 190, 192-194
Penrose, Roger, Sir, 334
Penzias, Arno, 149
Perimeter Institute for
Theoretical Physics, 327
perspective, 237
perturbation theory, 187
phantom energy, 274
phenomenology, 56
Philosophiae Naturalis
Principia Mathematica
(book), 73
phion field, 332
photoelectric effect, 102-104
photons
discovery of, 85
Feynman diagrams, 126
overview, 31
photoelectric effect,
102-104
release of, 128
studying GRBs, 219-220
physics. See also classical
physics; cosmology and
astrophysics; quantum
physics; Standard Model
of particle physics
high-energy, 56
laws of, 60-61
modern, birth of, 80
quantum, probability in,
111-112
theoretical, 55-56
two-time, 287-289
pions, 221
plagiarism, 85
Planck, Max, 85, 100, 102
Planck energy, 117-118
Planck length, 33,
117-118,328
Planck mass, 117
Planck scale energy, 136
Planck Surveyor
spacecraft, 214
Planck time, 117
Planck units, 116-118
Planck's constant, 100-102,
109, 331
plane geometry, 231
planetary model, 123-124
Planiverse, The (novel), 232
plasma, quark-gluon, 224
plurality of worlds, 263
pocket universes, 254
Pohl, Frederick, 293
Polchinski, Joe, 190-194, 348
Popper, Karl, 54
positive evidence, 53
positron, 127
postdiction, 211
potential energy, 66-67
pre-big bang models, 246
predictions, loop quantum
gravity, 317-318
predictive power, string
theory, 301
pre-geometric phase, 326
principles, scientific. See also
anthropic principle
conservation of mass, 29,
64-65
conservation of mass-
energy, 88
Copernican, 141-142
juO String Theory For Dummies _
principles, scientific
(continued)
cosmological, 143
of
of equivalence, 89-90
of falsifiability, 53-54
Feinberg reinterpretation, 290
holographic, 21,
197-200, 215
Pauli exclusion, 132
of relativity, 84
of speed of light, 84-86
of superposition, 70, 75
uncertainty, 34, 109-110,
272-273
probability, in quantum
physics, 111-112
projective geometry, 237
proof, of theories, 211
propagators, 126
proton decay, 217-218, 304
protons, 31-32, 129-131
Ptolemy, 139-140
pulsars, 220, 223
•5»
QED. See quantum
electrodynamics
quanta, 314
quantum chromodynamics
nucleons, 129-130
overview, 129
quarks, 130-131
twistor theory, 334
quantum computer, 333
quantum Einstein gravity,
324-326
quantum electrodynamics
(QED)
antimatter, 127-128
overview, 31, 125
particle information
exchange, 125-127
virtual particles, 128-129
quantum field theory
background-dependency, 279
overview, 10-11,41
QED, 126
virtual particles, 34
quantum foam, 33-34,
117,129
quantum gravity. See also
loop quantum gravity
background-dependence, 314
electromagnetism, 30-31
infinities, 33-34
laws of gravity, 26-28
matter, 29-30
nuclear forces, 31-32
overview, 10, 14, 18, 25
quantum jitters, 33-34
singularities, 33
supersymmetry, 174-176
unifying forces, 35-38
quantum information
theory, 333
quantum interpretation, 342
quantum jitters, 33-34
quantum mechanics, 272-274
quantum physics
applications of, 23
general relativity, 18
overview, 14
probability in, 111-112
quantum scale view of
matter, 29-30
quantum space bundles, 315
quantum states, 40
quantum theory
consistent histories
view, 115
Copenhagen
interpretation, 113
hidden variables
interpretation, 115-116
many worlds interpretation,
114-115
overview, 99-100
participatory anthropic
principle, 113-114
particles, 105-109
photons, 102-104
Planck units, 116-118
Planck's constant, 100-102
probability, 111-112
Schrodinger cat
experiment, 111-112
uncertainty principle,
109-110
waves, 105-109
quantum tunneling, 272-273
quantum wavefunction, 105,
108-109
quark-gluon plasma, 224
quarks, 32, 130-133, 217
qubit, 333
/?•
radioactive decay, 32
Ramanujan function, 163
Ramond, Pierre, 171, 177
Randall, Lisa, 203, 307, 349
Randall-Sundrum models,
202-204
rapid expansion, in inflation
theory, 152
realms, of universe, 138-139
redshift, 146
reductionism, 52
Rees, Martin, 258-259
reflection symmetry, 60
reinterpretation principle,
Feinberg, 290
Relativistic Heavy Ion
Collider (RHIC), 224
relativity. See also general
relativity; special
relativity
applying to mysteries of
universe, 95-96
ether, searching for, 82-83
Kaluza-Klein theory, 96-98
overview, 14, 81
principle of, 84
slowing time with, 281-282
time travel, 278-279
religion, concept of
multiverse in, 262
renormalization, 127,
136, 256
repulsive gravity, 154
Reuter, Martin, 325-326
revolution, scientific, 58-59
RHIC (Relativistic Heavy Ion
Collider), 224
Riemann, Bernhard, 236
Riemannian geometry, 163,
236-237
rogue universe, 274
rotating universe, 283
rotational symmetry, 60
Rovelli, Carlo, 317, 320
361
RSI model, 203
RS2 model, 203
Rubin, Vera, 153
Rutherford, Ernest, 123-124
Rutherford-Bohr model,
124-125
•5»
safety, asymptotic, 324-326
Sakai, Nobuyuki, 274
Salam, Abdus, 134
satellite, WMAP, 149, 155
Saturnian model, 123-124
Scalar-Tensor-Vector Gravity
(STVG), 332
Scherk, Joel, 173, 175-176
Schrodinger, Erwin, 108,
111-112
Schrodinger equation, 267
Schwarz, John, 171,175-177
346-347
Schwinger, Julian, 125
science
experimental falsifiability,
53-55
mathematics, 55-56
objectivity, 57
overview, 51
as revolution, 58-59
scientific method, 52-53
simplicity, rule of, 56-57
as symmetry, 60-62
as unification, 59-60
science fiction, 293
scientific method, 52-53
scientific paradigms, 58-59
scientific principles. See
principles, scientific
S-duality (strong-weak
duality), 184, 186-187
second law of motion, 73-74
simplicity, rule of, 56-57
singularities, 33, 95, 156
slowing time, with relativity
black hole event
horizons, 282
time dilation, 281-282
S-matrix, 162, 165-166
Smolin, Lee, 301, 305, 308,
310, 318-320
solar cells, 103
Somewhere in Time (film), 293
sound, 66
3-dimensional, 233-237
bending, 239-240
defining, 17-18
shortcuts through, 284-286
spacelike dimensions, 237
space-time
CDT, 325
dimensions of, 237-238
Einstein's theory of, 18, 28
fluidity, 309-310
loop quantum gravity, 319
moving through, 278-279
singularities, 33, 156
special relativity, 60
twister theory, 334
space-time continuum, 85, 87
sparticle (supersymmetric
particle), 172,212-213
special relativity
light, following bouncing
beam of, 85-87
mass and energy, unifying,
87-88
overview, 28, 84
science as unification, 60
space-time continuum,
building, 87
time dilation, 281
speed of light, 84-86, 330
spin, 36, 131, 168, 171,
241-242
spin network, 314-316,
319-320
spontaneous symmetry
breaking, 67-68
Standard Model of particle
physics
atomic theory, 120-125
versus bosonic string
theory, 165-166
bosons, 132
development of, 60
fermions, 132-133
gauge bosons, 133-134
hierarchy problem, 135-136
119
spontaneous symmetry
breaking, 68
supersymmetry, 37-38
theory of where mass
comes from, exploring,
134-135
unification, 35-36
standing wave, 71-72
start of universe
cyclic universe model, 247
ekpyrotic universe theory,
247-250
eternal universe, search
for, 246
overview, 245-246
states, quantum, 40
steady state theory, 147-148
Steinhardt, Paul, 265
stellar nucleosynthesis, 150
string theorists, criticism of,
305-308
string theory. See also
bosonic string theory;
testing string theory
aim of, 16-18
black holes, explaining
with, 40-41, 251-253
comebacks, 41-42
controversy, 297-311
disproving, 215-216
experimental complications
of, 46-47
finiteness of, 310-311
future complications, 46-47
gravity, predicting out of
strings, 40
heterotic strings, 180
implications of, 19-22
importance of, 22-23
key elements of, 12-16
versus loop quantum
gravity, 320-321
loss of interest in, 182
overview, 9-12
quantum field theory,
explaining, 41
setbacks, 43-45
start of universe, 245-250
Type I, 12-13, 179
TypellA, 179
TypellB, 179
j%}2 String Theory For Dummies _
string theory landscape, 45,
204-206
strings, 12-14
Strominger, Andrew,
192-194, 251
strong anthropic principle,
205-206
strong nuclear force, 14, 18
strong-weak duality
(S-duality), 184, 186-187
Structure of Scientific
Revolutions, The
(book), 58
STVG (Scalar-Tensor-Vector
Gravity), 332
supergravity, 176, 188-189
Super-Kamiokande neutrino
observatory, 217-218
supernovas, 150, 154
superpartners, 172-173,
212,343
superposition, principle of,
70,75
superstring revolution,
177-178, 188-189
superstring theories
bosons, 171-172
dimension problem,
173-174
fermions, 171-172
overview, 3
superpartners, 172-173
supersymmetry, 172-173
uniting five with two
dualities, 188-189
supersymmetric particle
(sparticle), 172, 212-213
supersymmetry
broken symmetry, 67
dark matter, 255
fundamental particles,
43-44
origins, 171
overview, 12, 15
quantum gravity, 37-38,
174-176
superpartners, 172-173
testing for, 210
testing implications of,
212-213
two-time physics, 289
Susskind, Leonard
anthropic principle, 207,
303-305
confirmation, 54-55
falsifiability, 54-55
holographic principle,
detecting with gravity
waves, 215
matrix theory, 196
overview, 347
string theory landscape,
45, 204
symmetry
broken, 213
conformal, 169
CPT, 277
internal, 67-68
overview, 64
scientific, 60-62
spontaneous symmetry
breaking, 68
translational, 67
T»
tachyons, 167-168, 290
Tau Zero (novel), 293
T-duality (topological
duality), 184-186
Tegmark, Max, 262-263
temporal mechanics
arrow of time, 276-278
chronology protection
conjecture, 279-280
space-time, moving
through, 278-279
tension, D-brane, 193
testing string theory
exploring universe, 219-223
obstacles to, 210-211
overview, 209
particle accelerators,
224-226
proton decay, 217-218
testing theories, 211
Texas sharpshooter
fallacy, 304
theoretical complications, of
string theory, 46
theoretical physics, 55-56
thermal energy, 66
thermodynamics, 29, 250-252
third law of motion, 74
Thomson, J.J., 122-123
Thorne, Kip, 285, 293
3-dimensional space
Mobius strip, 234-236
non-Euclidean geometry,
236-237
vectors, 233-234
time. See also time travel
arrow of, 276-278
asymmetries, 277
bending, 239-240
CDT, 325
defining, 17-18
dilation, 281-282
dimensions, 287-289
loop quantum gravity, 319
Planck, 117
sending messages
through, 290
shortcuts through, 284-286
symmetry, 344
time dilation, 87, 157, 280
Time Machine, The (novel),
232, 293
time travel
cosmic strings, crossing to
allow, 286-287
general relativity, 282-286
messages, sending through
time, 290
overview, 21, 275
paradoxes, 290-294
slowing time with relativity,
281-282
temporal mechanics,
276-280
time dimensions, 287-289
wormholes, 282-286
timelike dimensions, 237
Tipler, Frank, 114
Tomonaga, Sin-Itiro, 125
topological duality
(T-duality), 184-186
topology
cosmic, 240
study of, 185
toroidal duality, 185
torus, 16-17
Jndex 363
total energy, 66
Townsend, Paul, 189
translational symmetry,
transverse v\
Trouble with Physics, The
(book), 301, 305, 310,
318-319
trough, 69-70
true vacuum, 265
T-symmetry, 277
tunneling, quantum, 272-273
Turok, Neil, 327
twin paradox, 291
twistor space, 334
twistor theory, 334
2-dimensional brane
(2-brane), 13-14
2-dimensional space
Cartesian geometry,
231-233
Euclidean geometry, 231
two-time physics
adding new time dimension,
287-288
applications of, 289
overview, 287
reflecting onto one-time
Type HE string theory, 180
Type HO string theory, 180
Type I string theory,
12-13, 179
Type HA string theory, 179
Type IIB string theory, 179
•W»
ultraviolet catastrophe,
101-102
uncertainty principle, 34,
109-110,272-273
uncurling dimensions, 201
unification, scientific, 59-60
unified field theory, 35
unifying forces, 14, 18
unitarity, 267
universal gravitation, law
of, 74
universe. See also cosmology
and astrophysics;
parallel universes
accelerating expansion of,
44-45
causal dynamical
triangulations, 324-325
contraction of, 22
ekpyrotic, 21, 248-250,
256, 266
end of, 22, 344
eternal, 246, 318
evolution of, 253-256
expansion of, 143-146
exploring, 219-223
finely tuned, 258-260
heliocentric model, 141-142
as hologram, 21
incorrect models of,
138-140
internal relativity, 327
law of gravity, modifying,
328-332
mysteries of, applying
Einstein's work to, 95-96
noncommutative geometry,
334-335
one-time, reflecting two-
time physics onto,
288-289
overview, 323
pre-geometric phase, 326
quantum Einstein gravity,
325-326
quantum graphity, 326-327
quantum information
theory, 333
rotating, 283
start of, 245-250
string theory description
of, 309-311
symmetry, 61
twistor theory, 334
types of, 145
V
Vafa, Cumrun, 194, 203,
247-248, 251
van Nieuwenhuizen,
Peter, 176
van Stockum, W. J., 283
variable speed of light (VSL),
216, 329-331
vector spaces, 234
vectors, 233-234
velocity, wave, 70
Veneziano, Gabriele,
162-163, 246
Veneziano amplitude, 162
Veneziano model, 162
vibrational modes, 72
vibrations, 70-72
Vilenkin, Alex, 265
violating relativity, 215-216
Virgo Consortium research
group, 255
virtual particles, 34, 128-129
virtual photon, 126
Volkov, Dmitri, 171
von Neumann, John, 116
VSL (variable speed of light),
216, 329-331
W
, 41-43, 45
energy, 136, 343
W" bosons, 31
W* bosons, 31
wave interference, 70
wave packets, 164
wave particle duality, 105
wavefunction
decoherence, 113, 115
double split
experiment, 111
quantum, 105, 108-109
wavelength, 69-70
de Broglie hypothesis,
106-108
double slit experiment,
105-106
longitudinal, 169
overview, 69-70
quantum wavefunction,
108-109
standing, 71-72
jOu, String Theory For Dummies _
weak anthropic principle,
205-206
weak nuclear force, 14, 18
weak scale, 136
Weinberg, Steven, 134,
206, 259
Wells, H. G., 232, 293
Wess, Julius, 171
Wheeler, John Archibald, 113
white hole, 284
Wigner, Eugene, 269
Wilkinson Microwave
Anisotropy Probe
(WMAP) satellite,
149, 155
Wilson, Robert, 149
winding number, 185-186
Witten, Edward, 183-184,
188-189, 306, 334,
345-346
WMAP (Wilkinson Microwave
Anisotropy Probe)
satellite, 149, 155
Woit, Peter, 301
worldline, 87-88, 278-279
worlds, plurality of, 263
worldsheets, 87, 278-279
wormholes
accessing other universes,
271-272
negative energy,
overcoming instability
with, 286
overview, 20, 282-283
as shortcut through space
and time, 284-286
Wraparound Universe, The
(book), 240
Young, Thomas, 105
Z bosons, 31
Zeno's paradox, 118
Zumino, Bruno, 171
Zweig, George, 130
Zwicky, Fritz, 153
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Your plain-English guide to this
complex scientific theory
String theory is one of the most complicated sciences
being explored today. Not to worry though! This
informative guide clearly explains the basics of this hot
topic, discusses the theory's hypotheses and predictions,
and explores its curious implications. It also presents the
critical viewpoints in opposition to string theory so you can
draw your own conclusions.
• Understand the "theory of everything" — grasp the key concepts
and importance of the theory, and learn why scientists are so
excited about finding a theory of quantum gravity
• It all comes down to physics — discover how string theory is built
upon the major scientific developments of the early 20th century
• Building the theory — trace the creation and development of
string theory, discover its predictions, and see whether accurate
conclusions can be made
• Take string theory for a spin — explore the core issue of extra
dimensions, the implications for cosmology, and how string
theory could explain certain properties of our universe
• Boldly go where no one has gone — see what string theory has to
say about possible parallel universes, the origin and fate of our
universe, and the potential for time travel
• Hear from the critics — listen in on the heated debates about
string theory and weigh the alternatives being offered
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