M-theory: mother of all superstrings.
And Cumrun Vafa at Harvard has said, "I may be biased on this one, but I think it is perhaps the most important development not only in string theory, but also in theoretical physics at least in the past two decades." What is triggering all this excitement is the discovery of something called "M-theory," a theory that may explain the origin of strings. In one dazzling stroke, this new M-theory has solved some long-standing puzzling mysteries about string theory that have dogged it from the beginning, leaving many theoretical physicists (myself included!) gasping for breath. M-theory, moreover, may even force string theory to change its name. Although many features of M-theory are still unknown, it does not seem to be a theory purely of strings. Michael Duff of Texas A&M is already giving speeches with the title "The Theory Formerly Known as Strings!" String theorists are careful to point out that this does not prove the final correctness of the theory. Not by any means. That proof may take years or decades m ore. But it marks a most significant breakthrough that is already reshaping the entire field.
PARABLE OF THE LION
Einstein once said, "Nature shows us only the tail of the lion. But I do not doubt that the lion belongs to it even though he cannot at once reveal himself because of his enormous size." Einstein spent the last thirty years of his life searching for the "tail" that would lead him to the "lion," the fabled unified field theory or the "theory of everything," which would unite all the forces of the universe into a single equation. The four forces (gravity, electromagnetism, and the strong and weak nuclear forces) would be unified by an equation perhaps one inch long. Capturing the "lion" would be the greatest scientific achievement in all of physics, the crowning achievement of 2,000 years of scientific investigation, ever since the Greeks first asked themselves what the world was made of. But although Einstein was the first one to set off on this noble hunt and track the footprints left by the lion, he ultimately lost the trail and wandered off into the wilderness. Other giants of twentieth-century physics, suc h as Werner Heisenberg and Wolfgang Pauli, also joined in the hunt. But all the easy ideas were tried and shown to be wrong. When Niels Bohr once heard a lecture by Pauli explaining his version of the unified field theory, Bohr stood up and said, "We in the back are all agreed that your theory is crazy. But what divides us is whether your theory is crazy enough!"
The trail leading to the unified field theory, in fact, is littered with the wreckage of failed expeditions and dreams. Today, however, physicists are following a different trail that might be "crazy enough" to lead to the lion. This new trail leads to superstring theory, which is the best (and in fact only) candidate for a theory of everything. Unlike its rivals, it has survived every blistering mathematical challenge ever hurled at it. Not surprisingly, the theory is a radical, "crazy" departure from the past, being based on tiny strings vibrating in ten dimensional space-time. Moreover, the theory easily swallows up Einstein's theory of gravity. Witten has said, "Unlike conventional quantum field theory, string theory requires gravity. I regard this fact as one of the greatest insights in science ever made." But until recently, there has been a glaring weak spot: string theorists have been unable to probe all solutions of the model, failing miserably to examine what is called the "non-perturbative region," which I will describe shortly. This is vitally important because ultimately our universe (with its wonderfully diverse collection of galaxies, stars, planets, sub-atomic particles, and even people) may lie in this "non-perturbative region." Until this region can be probed, we don't know if string theory is a theory of everything -- or a theory of nothing! That's what today's excitement is all about. For the first time, using a powerful tool called "duality," physicists are now probing beyond just the tail, and finally seeing the outlines of a huge, unexpectedly beautiful lion at the other end. Not knowing what to call it, Witten has dubbed it "M-theory." In one stroke, M-theory has solved many of the embarrassing features of the theory, such as why we have five superstring theories. Ultimately, it may solve the nagging question of where strings come from.
PEA BRAINS AND THE MOTHER OF ALL STRINGS
Einstein once asked himself if God had any choice making the universe. Perhaps not, so it was embarrassing for string theorists to have five different self-consistent strings, all of which can unite the two fundamental theories in physics, the theory of gravity and the quantum theory.
Each of these string theories looks completely different from the others. They are based on different symmetries, with exotic names like E(8)xE(8) and 0(32).
Not only this, but superstrings are in some sense not unique: there are other non-string theories which contain "super-symmetry," the key mathematical symmetry underlying superstrings. (Changing light into electrons and then into gravity is one of the rather astonishing tricks performed by supersymmetry, which is the symmetry that can exchange particles with half-integral spin, such as electrons and quarks, with particles of integral spin, such as photons, gravitons, and W-particles.)
In eleven dimensions, in fact, there are alternate super theories based on membranes as well as point particles (called super-gravity). In lower dimensions, there is moreover a whole zoo of super theories based on membranes in different dimensions. (For example, point particles are zero-branes, strings are one-branes, membranes are two-branes, and so on.) For the p-dimensional case, some wag dubbed them p-branes (pronounced "pea brains"). But because pbranes are horribly difficult to work with, they were long considered just a historical curiosity, a trail that led to a dead-end. (Michael Duff, in fact, has collected a whole list of unflattering comments made by referees to his National Science Foundation grant concerning his work on p-branes. One of the more charitable comments from a referee was: "He has a skewed view of the relative importance of various concepts in modern theoretical physics.") So that was the mystery. Why should supersymmetry allow for five superstrings and this peculiar, motley collecti on of p-branes? Now we realize that strings, super-gravity, and p-branes are just different aspects of the same theory. M-theory (M for "membrane" or the "mother of all strings," take your pick) unites the five superstrings into one theory and includes the pbranes as well. To see how this all fits together, let us update the famous parable of the blind men and the elephant. Think of the blind men on the trail of the lion. Hearing it race by, they chase after it and desperately grab onto its tail (a one-brane). Hanging onto the tail for dear life, they feel its one-dimensional form and loudly proclaim "It's a string! It's a string!"
But then one blind man goes beyond the tail and grabs onto the ear of the lion. Feeling a two-dimensional surface (a membrane), the blind man proclaims, "No, it's really a two-brane!" Then another blind man is able to grab onto the leg of the lion. Sensing a three-dimensional solid, he shouts, "No, you're both wrong. It's really a three-brane!" Actually, they are all right. Just as the tail, ear, and leg are different parts of the same lion, the string and various p-branes appear to be different limits of the same theory: M-theory. Paul Townsend of Cambridge University, one of the architects of this idea, calls it "p-brane democracy"; that is, all p-branes (including strings) are created equal. Schwarz puts a slightly different spin on this. He says, "We are in an Orwellian situation: all p-branes are equal, but some (namely strings) are more equal than others. The point is that they are the only ones on which we can base a perturbation theory." To understand unfamiliar concepts such as duality, perturbation theory, and non-perturbative solutions, it is instructive to see where these concepts first entered into physics.
The key tool to understanding this breakthrough is something called "duality." Loosely speaking, two theories are "dual" to each other if they can be shown to be equivalent under a certain interchange. The simplest example of duality is reversing the role of electricity and magnetism in the equations discovered by James Clerk Maxwell of Cambridge University 130 years ago. These are the equations that govern light, television, X-rays, radar, dynamos, motors, transformers, even the Internet and computers. The remarkable feature about these equations is that they remain the same if we interchange the magnetic field B and electric field E and also switch the electric charge "e" with the magnetic charge "g" of a magnetic "monopole": E [left and right arrow] B and e [left and right arrow] g (In fact, the product "eg" is a constant.) This has important implications. Often, when a theory cannot be solved exactly, we use an approximation scheme. In first-year calculus, for example, we recall that we can approximate ce rtain functions by Taylor's expansion. Similarly, since [e.sup.2] = 1/137 in certain units and is hence a small number, we can always approximate the theory by power expanding in [e.sup.2]. So we add contributions of order [e.sup.2] + [e.sup.4] + [e.sup.6] and so on in solving for, say, the collision of two particles. Notice that each contribution is getting smaller and smaller, so we can in principle add them all up. This generalization of Taylor's expansion is called "perturbation theory," where we perturb the system with terms containing [e.sup.2]. For example, in archery, perturbation theory is how we aim our arrows. With every motion of our arms, our bow gets closer and closer to aligning with the bull's eye. But now try expanding in [g.sup.2]. This is much tougher; in fact, if we expand in [g.sup.2], which is large, then the sum [g.sup.2] + [g.sup.4] + [g.sup.6] etc. blows up and becomes meaningless. This is the reason why the "non-perturbative" region is so difficult to probe, since the theory simply b lows up if we try to naively use perturbation theory for large coupling constant g. So at first it appears hopeless that we could ever penetrate into the non-perturbative region. (For example, if every motion of our arms got bigger and bigger, we would never be able to zero in and hit the target with the arrow.) But notice that because of duality, a theory of e (which is easily solved) is identical to a theory of large g (which is difficult to solve). Because they are the same theory, we can use duality to solve for the non-perturbative region.
S, T, AND U DUALITY
The first inkling that duality might apply in string theory was discovered by K. Kikkawa and M. Yamasaki of Osaka University in 1984. They showed that if you "curled up" one of the extra dimensions into a circle with radius R, the theory was the same if we curled up this dimension with radius 1/R. This is now called T duality: R [left and right arrow] l/R When applied to various superstrings, one could reduce five of the string theories to three. In nine dimensions (with one dimension curled up) the Type IIa and IIb strings were identical, as were the E(8)xE(8) and O(32) strings.
Unfortunately, T duality was still a perturbative duality. The next breakthrough came when it was shown that there was a second class of dualities, called S duality, which provided a duality between the perturbative and non-perturbative regions of string theory. Another duality, called U duality, was even more powerful.
Then Nathan Seiberg and Witten brilliantly showed how another form of duality could solve for the non-perturbative region in four dimensional supersymmetric theories. However, what finally convinced many physicists of the power of this technique was the work of Edward Witten and Paul Townsend. They caught everyone by surprise by showing that there was a duality between ten dimensional Type IIa strings and eleven dimensional supergravity! The non-perturbative region of Type IIa strings, which was previously a forbidden region, was revealed to be governed by eleven dimensional supergravity theory, with one dimension curled up. At this point, I remember that many physicists (me included) were rubbing our eyes, not believing what we were seeing. I remember saying to myself, "But that's impossible!"
All of a sudden, we realized that perhaps the real "home" of string theory was not ten dimensions, but possibly eleven, and that the theory wasn't fundamentally a string theory at all! This revived tremendous interest in eleven dimensional theories and p-branes. Lurking in the eleventh dimension was an entirely new theory which could reduce to eleven dimensional supergravity as well as ten dimensional string theory and p-brane theory.
DETRACTORS OF STRING THEORIES
To the critics, however, these mathematical developments still don't answer the nagging question: How do you test it? Because string theory is really a theory of Creation, when all its beautiful symmetries were in their full glory, the only way to test it, the critics wail, is to recreate the Big Bang itself, which is impossible. Nobel Laureate Sheldon Glashow likes to ridicule superstring theory by comparing it with former President Reagan's Star Wars plan, that is, they are both untestable, soak up resources, and siphon off the best scientific brains.
Actually, most string theorists think these criticisms are silly. They believe that the critics have missed the point. The key point is this: if the theory can be solved non-perturbatively using pure mathematics, then it should reduce at low energies to a theory of ordinary protons, electrons, atoms, and molecules, for which there is ample experimental data. If we could completely solve the theory, we should be able to extract its low-energy spectrum, which should match the familiar particles we see today in the Standard Model. Thus, the problem is not building atom smashers 1,000 light years in diameter; the real problem is raw brain power: if only we were clever enough, we could write down M-theory, solve it, and settle everything.
So what would it take to actually solve the theory once and for all and end all the speculation and back-biting? There are several approaches. The first is the most direct: try to derive the Standard Model of particle interactions, with its bizarre collection of quarks, gluons, electrons, neutrinos, Riggs bosons, etc. etc. etc. (I must admit that although the Standard Model is the most successful physical theory ever proposed, it is also one of the ugliest.) This might be done by curling up six of the ten dimensions, leaving us with a four dimensional theory that might resemble the Standard Model a bit, then try to use duality and M-theory to probe its non-perturbative region, seeing if the symmetries break in the correct fashion, giving us the correct masses of the quarks and other particles in the Standard Model. Witten's philosophy, however, is a bit different. He feels that the key to solving string theory is to understand the underlying principle behind the theory.
Let me explain. Einstein's theory of general relativity, for example, started from first principles. Einstein had the "happiest thought in his life" when he leaned back in his chair at the Bern patent office and realized that a person in a falling elevator would feel no gravity. Although physicists since Galileo knew this, Einstein was able to extract from this the Equivalence Principle. This deceptively simple statement (that the laws of physics are indistinguishable locally in an accelerating or a gravitating frame) led Einstein to introduce a new symmetry to physics, general coordinate transformations. This in turn gave birth to the action principle behind general relativity, the most beautiful and compelling theory of gravity. Only now are we trying to quantize the theory to make it compatible with the other forces. So the evolution of this theory can be summarized as: Principle Symmetry -----> Action -----> Quantum Theory.
According to Witten, we need to discover the analog of the Equivalence Principle for string theory. The fundamental problem has been that string theory has been evolving "backwards." As Witten says, "string theory is twenty-first-century physics which fell into the twentieth century by accident." We were never "meant" to see this theory until the next century.
IS THE END IN SIGHT?
Vafa recently added a strange twist to this when he introduced yet another mega-theory, this time a twelve-dimensional theory called F-theory (F for "father") which explains the self-duality of the IIb string. (Unfortunately, this twelve-dimensional theory is rather strange: it has two time coordinates, not one, and actually violates twelve-dimensional relativity. Imagine trying to live in a world with two times! It would put an episode of Twilight Zone to shame.) So is the final theory ten, eleven, or twelve dimensional?
Schwarz, for one, feels that the final version of M-theory may not even have any fixed dimension. He feels that the true theory may be independent of any dimensionality of space-time, and that eleven dimensions only emerge once one tries to solve it. Townsend seems to agree, saying "the whole notion of dimensionality is an approximate one that only emerges in some semi-classical context." So does this mean that the end is in sight, that we will someday soon derive the Standard Model from first principles? I asked some of the leaders in this field to respond to this question. Although they are all enthusiastic supporters of this revolution, they are still cautious about predicting the future. Townsend believes that we are in a stage similar to the old quantum era of the Bohr atom, just before the full elucidation of quantum mechanics. He says, "We have some fruitful pictures and some rules analogous to the Bohr-Sommerfeld quantization rules, but it's also clear that we don't have a complete theory."
Duff says, "Is M-theory merely a theory of super-membranes and super S-branes requiring some (as yet unknown) non-perturbative quantization, or (as Witten believes) are the underlying degrees of freedom of M-theory yet to be discovered? I am personally agnostic on this point." Witten certainly believes we are on the right track, but we need a few more "revolutions" like this to finally solve the theory. "I think there are still a couple more superstring revolutions in our future, at least. If we can manage one more super string revolution a decade, I think that we will do all right," he says. Vafa says, "I hope this is the 'light at the end of the tunnel' but who knows how long the tunnel is!" Schwarz, moreover, has written about M-theory: "Whether it is based on something geometrical (like supermembranes) or something completely different is still not known. In any case, finding it would be a landmark in human intellectual history." Personally, I am optimistic. For the first time, we can see the outline of t he lion, and it is magnificent. One day, we will hear it roar.
Michio Kaku is professor of theoretical physics at the City University of New York. He is author of numerous books, including Hyperspace (1994), Beyond Einstein (1995), Visions (1997), and Introduction to Superstings and M-theory (1999). His web site is www.mkaku.org.
A version of this article was first published in the January 18, 1997 issue of the New Scientist. Reprinted by permission.
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|Publication:||Phi Kappa Phi Forum|
|Date:||Sep 22, 2002|
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