String theory
String theory 

Fundamental objects 
Perturbative theory 
Nonperturbative results 
Phenomenology 
Mathematics 
Theorists

In physics, string theory is a theoretical framework in which the pointlike particles of particle physics are replaced by onedimensional objects called strings.^{[1]} String theory aims to explain all types of observed elementary particles using quantum states of these strings. In addition to the particles postulated by the standard model of particle physics, string theory naturally incorporates gravity and so is a candidate for a theory of everything, a selfcontained mathematical model that describes all fundamental forces and forms of matter. Besides this potential role, string theory is now widely used as a theoretical tool and has shed light on many aspects of quantum field theory and quantum gravity.^{[2]}
The earliest version of string theory, bosonic string theory, incorporated only the class of particles known as bosons. It was then developed into superstring theory, which posits that a connection – a "supersymmetry" – exists between bosons and the class of particles called fermions. String theory requires the existence of extra spatial dimensions for its mathematical consistency. In realistic physical models constructed from string theory, these extra dimensions are typically compactified to extremely small scales.
String theory was first studied in the late 1960s^{[3]} as a theory of the strong nuclear force before being abandoned in favor of the theory of quantum chromodynamics. Subsequently, it was realized that the very properties that made string theory unsuitable as a theory of nuclear physics made it a promising candidate for a quantum theory of gravity. Five consistent versions of string theory were developed until it was realized in the mid1990s that they were different limits of a conjectured single 11dimensional theory now known as Mtheory.^{[4]}
Many theoretical physicists, including Stephen Hawking, Edward Witten and Juan Maldacena, believe that string theory is a step towards the correct fundamental description of nature: it accommodates a consistent combination of quantum field theory and general relativity, agrees with insights in quantum gravity (such as the holographic principle and black hole thermodynamics) and has passed many nontrivial checks of its internal consistency.^{[citation needed]} According to Hawking, "Mtheory is the only candidate for a complete theory of the universe."^{[5]} Other physicists, such as Richard Feynman,^{[6]}^{[7]} Roger Penrose^{[8]} and Sheldon Lee Glashow,^{[9]} have criticized string theory for not providing novel experimental predictions at accessible energy scales.
Contents
Overview
The starting point for string theory is the idea that the pointlike particles of elementary particle physics can also be modeled as onedimensional objects called strings. According to string theory, strings can oscillate in many ways. On distance scales larger than the string radius, each oscillation mode gives rise to a different species of particle, with its mass, charge, and other properties determined by the string's dynamics. Splitting and recombination of strings correspond to particle emission and absorption, giving rise to the interactions between particles. An analogy for strings' modes of vibration is a guitar string's production of multiple distinct musical notes.^{[clarification needed]} In this analogy, different notes correspond to different particles.
In string theory, one of the modes of oscillation of the string corresponds to a massless, spin2 particle. Such a particle is called a graviton since it mediates a force which has the properties of gravity. Since string theory is believed to be a mathematically consistent quantum mechanical theory, the existence of this graviton state implies that string theory is a theory of quantum gravity.
String theory includes both open strings, which have two distinct endpoints, and closed strings, which form a complete loop. The two types of string behave in slightly different ways, yielding different particle types. For example, all string theories have closed string graviton modes, but only open strings can correspond to the particles known as photons. Because the two ends of an open string can always meet and connect, forming a closed string, all string theories contain closed strings.
The earliest string model, the bosonic string, incorporated only the class of particles known as bosons. This model describes, at low enough energies, a quantum gravity theory, which also includes (if open strings are incorporated as well) gauge bosons such as the photon. However, this model has problems. What is most significant is that the theory has a fundamental instability, believed to result in the decay (at least partially) of spacetime itself. In addition, as the name implies, the spectrum of particles contains only bosons, particles which, like the photon, obey particular rules of behavior. Roughly speaking, bosons are the constituents of radiation, but not of matter, which is made of fermions. Investigating how a string theory may include fermions led to the invention of supersymmetry, a mathematical relation between bosons and fermions. String theories that include fermionic vibrations are now known as superstring theories; several kinds have been described, but all are now thought to be different limits of a theory called Mtheory.
Since string theory incorporates all of the fundamental interactions, including gravity, many physicists hope that it fully describes our universe, making it a theory of everything. One of the goals of current research in string theory is to find a solution of the theory that is quantitatively identical with the standard model, with a small cosmological constant, containing dark matter and a plausible mechanism for cosmic inflation. It is not yet known whether string theory has such a solution, nor is it known how much freedom the theory allows to choose the details.
One of the challenges of string theory is that the full theory does not yet have a satisfactory definition in all circumstances. The scattering of strings is most straightforwardly defined using the techniques of perturbation theory, but it is not known in general how to define string theory nonperturbatively. It is also not clear as to whether there is any principle by which string theory selects its vacuum state, the spacetime configuration that determines the properties of our universe (see string theory landscape).
Strings
The motion of a pointlike particle can be described by drawing a graph of its position with respect to time. The resulting picture depicts the worldline of the particle in spacetime. In an analogous way, one can draw a graph depicting the progress of a string as time passes. The string, which looks like a small line by itself, will sweep out a twodimensional surface known as the worldsheet. The different string modes (giving rise to different particles, such as the photon or graviton) appear as waves on this surface.
A closed string looks like a small loop, so its worldsheet will look like a pipe. An open string looks like a segment with two endpoints, so its worldsheet will look like a strip. In a more mathematical language, these are both Riemann surfaces, the strip having a boundary and the pipe none.
Strings can join and split. This is reflected by the form of their worldsheet, or more precisely, by its topology. For example, if a closed string splits, its worldsheet will look like a single pipe splitting into two pipes. This topology is often referred to as a pair of pants (see drawing at right). If a closed string splits and its two parts later reconnect, its worldsheet will look like a single pipe splitting to two and then reconnecting, which also looks like a torus connected to two pipes (one representing the incoming string, and the other representing the outgoing one). An open string doing the same thing will have a worldsheet that looks like an annulus connected to two strips.
In quantum mechanics, one computes the probability for a point particle to propagate from one point to another by summing certain quantities called probability amplitudes. Each amplitude is associated with a different worldline of the particle. This process of summing amplitudes over all possible worldlines is called path integration. In string theory, one computes probabilities in a similar way, by summing quantities associated with the worldsheets joining an initial string configuration to a final configuration. It is in this sense that string theory extends quantum field theory, replacing point particles by strings. As in quantum field theory, the classical behavior of fields is determined by an action functional, which in string theory can be either the Nambu–Goto action or the Polyakov action.
Branes
In string theory and related theories such as supergravity theories, a brane is a physical object that generalizes the notion of a point particle to higher dimensions.^{[10]} For example, a point particle can be viewed as a brane of dimension zero, while a string can be viewed as a brane of dimension one. It is also possible to consider higherdimensional branes. In dimension p, these are called pbranes. The word brane comes from the word "membrane" which refers to a twodimensional brane.
Branes are dynamical objects which can propagate through spacetime according to the rules of quantum mechanics. They have mass and can have other attributes such as charge. A pbrane sweeps out a (p+1)dimensional volume in spacetime called its worldvolume. Physicists often study fields analogous to the electromagnetic field which live on the worldvolume of a brane.
In string theory, Dbranes are an important class of branes that arise when one considers open strings. As an open string propagates through spacetime, its endpoints are required to lie on a Dbrane. The letter "D" in Dbrane refers to the fact that we impose a certain mathematical condition on the system known as the Dirichlet boundary condition. The study of Dbranes in string theory has led to important results such as the AdS/CFT correspondence, which has shed light on many problems in quantum field theory.
Branes are also frequently studied from a purely mathematical point of view^{[11]} since they are related to subjects such as homological mirror symmetry and noncommutative geometry. Mathematically, branes may be represented as objects of certain categories, such as the derived category of coherent sheaves on a Calabi–Yau manifold, or the Fukaya category.
Dualities
In physics, the term duality refers to a situation where two seemingly different physical systems turn out to be equivalent in a nontrivial way. If two theories are related by a duality, it means that one theory can be transformed in some way so that it ends up looking just like the other theory. The two theories are then said to be dual to one another under the transformation. Put differently, the two theories are mathematically different descriptions of the same phenomena.
In addition to providing a candidate for a theory of everything, string theory provides many examples of dualities between different physical theories and can therefore be used as a tool for understanding the relationships between these theories.^{[12]}
S, T, and Uduality
These are dualities between string theories which relate seemingly different quantities. Large and small distance scales, as well as strong and weak coupling strengths, are quantities that have always marked very distinct limits of behavior of a physical system in both classical and quantum physics. But strings can obscure the difference between large and small, strong and weak, and this is how these five very different theories end up being related. Tduality relates the large and small distance scales between string theories, whereas Sduality relates strong and weak coupling strengths between string theories. Uduality links Tduality and Sduality.
Mtheory
Before the 1990s, string theorists believed there were five distinct superstring theories: type I, type IIA, type IIB, and the two flavors of heterotic string theory (SO(32) and E_{8}×E_{8}). The thinking was that out of these five candidate theories, only one was the actual correct theory of everything, and that theory was the one whose low energy limit, with ten spacetime dimensions compactified down to four, matched the physics observed in our world today. It is now believed that this picture was incorrect and that the five superstring theories are related to one another by the dualities described above. The existence of these dualities suggests that the five string theories are in fact special cases of a more fundamental theory called Mtheory.^{[13]}
Type  Spacetime dimensions  Details 

Bosonic  26  Only bosons, no fermions, meaning only forces, no matter, with both open and closed strings; major flaw: a particle with imaginary mass, called the tachyon, representing an instability in the theory. 
I  10  Supersymmetry between forces and matter, with both open and closed strings; no tachyon; gauge group is SO(32) 
IIA  10  Supersymmetry between forces and matter, with only closed strings; no tachyon; massless fermions are nonchiral 
IIB  10  Supersymmetry between forces and matter, with only closed strings; no tachyon; massless fermions are chiral 
HO  10  Supersymmetry between forces and matter, with closed strings only; no tachyon; heterotic, meaning right moving and left moving strings differ; gauge group is SO(32) 
HE  10  Supersymmetry between forces and matter, with closed strings only; no tachyon; heterotic; gauge group is E_{8}×E_{8} 
Extra dimensions
Number of dimensions
An intriguing feature of string theory is that it predicts extra dimensions. In classical string theory the number of dimensions is not fixed by any consistency criterion. However, to make a consistent quantum theory, string theory is required to live in a spacetime of the socalled "critical dimension": we must have 26 spacetime dimensions for the bosonic string and 10 for the superstring. This is necessary to ensure the vanishing of the conformal anomaly of the worldsheet conformal field theory. Modern understanding indicates that there exist less trivial ways of satisfying this criterion. Cosmological solutions exist in a wider variety of dimensionalities, and these different dimensions are related by dynamical transitions. The dimensions are more precisely different values of the "effective central charge", a count of degrees of freedom that reduces to dimensionality in weakly curved regimes.^{[14]}^{[15]}
One such theory is the 11dimensional Mtheory, which requires spacetime to have eleven dimensions,^{[16]} as opposed to the usual three spatial dimensions and the fourth dimension of time. The original string theories from the 1980s describe special cases of Mtheory where the eleventh dimension is a very small circle or a line, and if these formulations are considered as fundamental, then string theory requires ten dimensions. But the theory also describes universes like ours, with four observable spacetime dimensions, as well as universes with up to 10 flat space dimensions, and also cases where the position in some of the dimensions is described by a complex number rather than a real number. The notion of spacetime dimension is not fixed in string theory: it is best thought of as different in different circumstances.^{[17]}
Nothing in Maxwell's theory of electromagnetism or Einstein's theory of relativity makes this kind of prediction; these theories require physicists to insert the number of dimensions manually and arbitrarily, and this number is fixed and independent of potential energy. String theory allows one to relate the number of dimensions to scalar potential energy. In technical terms, this happens because a gauge anomaly exists for every separate number of predicted dimensions, and the gauge anomaly can be counteracted by including nontrivial potential energy into equations to solve motion. Furthermore, the absence of potential energy in the "critical dimension" explains why flat spacetime solutions are possible.
This can be better understood by noting that a photon included in a consistent theory (technically, a particle carrying a force related to an unbroken gauge symmetry) must be massless. The mass of the photon that is predicted by string theory depends on the energy of the string mode that represents the photon. This energy includes a contribution from the Casimir effect, namely from quantum fluctuations in the string. The size of this contribution depends on the number of dimensions, since for a larger number of dimensions there are more possible fluctuations in the string position. Therefore, the photon in flat spacetime will be massless—and the theory consistent—only for a particular number of dimensions.^{[18]} When the calculation is done, the critical dimensionality is not four as one may expect (three axes of space and one of time). The subset of X is equal to the relation of photon fluctuations in a linear dimension. Flat space string theories are 26dimensional in the bosonic case, while superstring and Mtheories turn out to involve 10 or 11 dimensions for flat solutions. In bosonic string theories, the 26 dimensions come from the Polyakov equation.^{[19]} Starting from any dimension greater than four, it is necessary to consider how these are reduced to fourdimensional spacetime.
Compact dimensions
Two ways have been proposed to resolve this apparent contradiction. The first is to compactify the extra dimensions; i.e., the 6 or 7 extra dimensions are so small as to be undetectable by presentday experiments.
To retain a high degree of supersymmetry, these compactification spaces must be very special, as reflected in their holonomy. A 6dimensional manifold must have SU(3) structure, a particular case (torsionless) of this being SU(3) holonomy, making it a Calabi–Yau space, and a 7dimensional manifold must have G_{2} structure, with G_{2} holonomy again being a specific, simple, case. Such spaces have been studied in attempts to relate string theory to the 4dimensional Standard Model, in part due to the computational simplicity afforded by the assumption of supersymmetry. More recently, progress has been made constructing more realistic compactifications without the degree of symmetry of Calabi–Yau or G2 manifolds.^{[citation needed]}
A standard analogy for this is to consider multidimensional space as a garden hose. If the hose is viewed from sufficient distance, it appears to have only one dimension, its length. Indeed, think of a ball just small enough to enter the hose. Throwing such a ball inside the hose, the ball would move more or less in one dimension; in any experiment we make by throwing such balls in the hose, the only important movement will be onedimensional, that is, along the hose. However, as one approaches the hose, one discovers that it contains a second dimension, its circumference. Thus, an ant crawling inside it would move in two dimensions (and a fly flying in it would move in three dimensions). This "extra dimension" is only visible within a relatively close range to the hose, or if one "throws in" small enough objects. Similarly, the extra compact dimensions are only "visible" at extremely small distances, or by experimenting with particles with extremely small wavelengths (of the order of the compact dimension's radius), which in quantum mechanics means very high energies (see wave–particle duality).
Braneworld scenario
Another possibility is that we are "stuck" in a 3+1 dimensional (three spatial dimensions plus one time dimension) subspace of the full universe. Properly localized matter and Yang–Mills gauge fields will typically exist if the subspacetime is an exceptional set of the larger universe.^{[20]} These "exceptional sets" are ubiquitous in Calabi–Yau nfolds and may be described as subspaces without local deformations, akin to a crease in a sheet of paper or a crack in a crystal, the neighborhood of which is markedly different from the exceptional subspace itself. However, until the work of Randall and Sundrum,^{[21]} it was not known that gravity can be properly localized to a subspacetime. In addition, spacetime may be stratified, containing strata of various dimensions, allowing us to inhabit the 3+1dimensional stratum—such geometries occur naturally in Calabi–Yau compactifications.^{[22]} Such subspacetimes are Dbranes, hence such models are known as braneworld scenarios.
In either case, gravity acting in the hidden dimensions affects other nongravitational forces such as electromagnetism. In fact, Kaluza's early work demonstrated that general relativity in five dimensions actually predicts the existence of electromagnetism. However, because of the nature of Calabi–Yau manifolds, no new forces appear from the small dimensions, but their shape has a profound effect on how the forces between the strings appear in our fourdimensional universe. In principle, therefore, it is possible to deduce the nature of those extra dimensions by requiring consistency with the standard model, but this is not yet a practical possibility. It is also possible to extract information regarding the hidden dimensions by precision tests of gravity, but so far these have only put upper limitations on the size of such hidden dimensions.
Testability and experimental predictions
Although a great deal of recent work has focused on using string theory to construct realistic models of particle physics, several major difficulties complicate efforts to test models based on string theory. The most significant is the extremely small size of the Planck length, which is expected to be close to the string length (the characteristic size of a string, where strings become easily distinguishable from particles). Another issue is the huge number of metastable vacua of string theory, which might be sufficiently diverse to accommodate almost any phenomena we might observe at lower energies.
String harmonics
One unique prediction of string theory is the existence of string harmonics. At sufficiently high energies, the stringlike nature of particles would become obvious. There should be heavier copies of all particles, corresponding to higher vibrational harmonics of the string. It is not clear how high these energies are. In most conventional string models, they would be close to the Planck energy, which is 10^{14} times higher than the energies accessible in the newest particle accelerator, the LHC, making this prediction impossible to test with any particle accelerator in the near future. However, in models with large extra dimensions they could potentially be produced at the LHC, or at energies not far above its reach.
Cosmology
String theory as currently understood makes a series of predictions for the structure of the Universe at the largest scales. Many phases in string theory have very large, positive vacuum energy.^{[23]} Regions of the Universe that are in such a phase will inflate exponentially rapidly in a process known as eternal inflation. As such, the theory predicts that most of the Universe is very rapidly expanding. However, these expanding phases are not stable, and can decay via the nucleation of bubbles of lower vacuum energy. Since our local region of the Universe is not very rapidly expanding, string theory predicts we are inside such a bubble. The spatial curvature of the "universe" inside the bubbles that form by this process is negative, a testable prediction.^{[24]} Moreover, other bubbles will eventually form in the parent vacuum outside the bubble and collide with it. These collisions lead to potentially observable imprints on cosmology.^{[25]} However, it is possible that neither of these will be observed if the spatial curvature is too small and the collisions are too rare.
Under certain circumstances, fundamental strings produced at or near the end of inflation can be "stretched" to astronomical proportions. These cosmic strings could be observed in various ways, for instance by their gravitational lensing effects. However, certain field theories also predict cosmic strings arising from topological defects in the field configuration.^{[26]}
Supersymmetry
If confirmed experimentally, supersymmetry is often considered circumstantial evidence, because most consistent string theories are spacetime supersymmetric. As with other physical theories, the existence of spacetime supersymmetry is a desired feature addressing various issues we encounter in nonsupersymmetric theories, like in the Standard Model. However, the absence of supersymmetric particles at energies accessible to the LHC will not actually disprove string theory, since the energy scale at which supersymmetry is broken could be well above the accelerator's range. This would make supersymmetric particles too heavy to be produced in relatively lower energies. On the other hand, there are fully consistent nonsupersymmetric stringtheories that can also provide phenomenologically relevant predictions.
AdS/CFT correspondence
The antide Sitter/conformal field theory (AdS/CFT) correspondence is a relationship which says that string theory is in certain cases equivalent to a quantum field theory. More precisely, one considers string or Mtheory on an antide Sitter background. This means that the geometry of spacetime is obtained by perturbing a certain solution of Einstein's equation in the vacuum. In this setting, it is possible to define a notion of "boundary" of spacetime. The AdS/CFT correspondence states that this boundary can be regarded as the "spacetime" for a quantum field theory, and this field theory is equivalent to the bulk gravitational theory in the sense that there is a "dictionary" for translating calculations in one theory into calculations in the other.
Examples of the correspondence
The most famous example of the AdS/CFT correspondence states that Type IIB string theory on the product AdS_{5} × S^{5} is equivalent to N = 4 super Yang–Mills theory on the fourdimensional conformal boundary.^{[27]}^{[28]}^{[29]}^{[30]} Another realization of the correspondence states that Mtheory on AdS_{4} × S^{7} is equivalent to the ABJM superconformal field theory in three dimensions.^{[31]} Yet another realization states that Mtheory on AdS_{7} × S^{4}is equivalent to the socalled (2,0)theory in six dimensions.^{[32]}
Applications to quantum chromodynamics
Since it relates string theory to ordinary quantum field theory, the AdS/CFT correspondence can be used as a theoretical tool for doing calculations in quantum field theory. For example, the correspondence has been used to study the quark–gluon plasma, an exotic state of matter produced in particle accelerators.
The physics of the quark–gluon plasma is governed by quantum chromodynamics, the fundamental theory of the strong nuclear force, but this theory is mathematically intractable in problems involving the quark–gluon plasma. In order to understand certain properties of the quark–gluon plasma, theorists have therefore made use of the AdS/CFT correspondence. One version of this correspondence relates string theory to a certain supersymmetric gauge theory called N = 4 super Yang–Mills theory. The latter theory provides a good approximation to quantum chromodynamics. One can thus translate problems involving the quark–gluon plasma into problems in string theory which are more tractable. Using these methods, theorists have computed the shear viscosity of the quark–gluon plasma.^{[33]} In 2008, these predictions were confirmed at the Relativistic Heavy Ion Collider at Brookhaven National Laboratory.^{[34]}
Applications to condensed matter physics
In addition, string theory methods have been applied to problems in condensed matter physics. Certain condensed matter systems are difficult to understand using the usual methods of quantum field theory, and the AdS/CFT correspondence may allow physicists to better understand these systems by describing them in the language of string theory. Some success has been achieved in using string theory methods to describe the transition of a superfluid to an insulator.^{[35]}^{[36]}
Connections to mathematics
In addition to influencing research in theoretical physics, string theory has stimulated a number of major developments in pure mathematics. Like many developing ideas in theoretical physics, string theory does not at present have a mathematically rigorous formulation in which all of its concepts can be defined precisely. As a result, physicists who study string theory are often guided by physical intuition to conjecture relationships between the seemingly different mathematical structures that are used to formalize different parts of the theory. These conjectures are later proved by mathematicians, and in this way, string theory has served as a source of new ideas in pure mathematics.^{[37]}
Mirror symmetry
One of the ways in which string theory influenced mathematics was through the discovery of mirror symmetry. In string theory, the shape of the unobserved spatial dimensions is typically encoded in mathematical objects called Calabi–Yau manifolds. These are of interest in pure mathematics, and they can be used to construct realistic models of physics from string theory. In the late 1980s, it was noticed that given such a physical model, it is not possible to uniquely reconstruct a corresponding Calabi–Yau manifold. Instead, one finds that there are two Calabi–Yau manifolds that give rise to the same physics. These manifolds are said to be "mirror" to one another. The existence of this mirror symmetry relationship between different Calabi–Yau manifolds has significant mathematical consequences as it allows mathematicians to solve many problems in enumerative algebraic geometry. Today mathematicians are still working to develop a mathematical understanding of mirror symmetry based on physicists' intuition.^{[38]}
Vertex operator algebras
In addition to mirror symmetry, applications of string theory to pure mathematics include results in the theory of vertex operator algebras. For example, ideas from string theory were used by Richard Borcherds in 1992 to prove the monstrous moonshine conjecture relating the monster group (a construction arising in group theory, a branch of algebra) and modular functions (a class of functions which are important in number theory).^{[39]}
History
This section does not cite any sources. (February 2013) (Learn how and when to remove this template message) 
Early results
Some of the structures reintroduced by string theory arose for the first time much earlier as part of the program of classical unification started by Albert Einstein. The first person to add a fifth dimension to a theory of gravity was Gunnar Nordström in 1914, who noted that gravity in five dimensions describes both gravity and electromagnetism in four. Nordström attempted to unify electromagnetism with his theory of gravitation, which was however superseded by Einstein's general relativity in 1919.^{[40]} Thereafter, German mathematician Theodor Kaluza combined the fifth dimension with general relativity, and only Kaluza is usually credited with the idea.^{[40]} In 1926, the Swedish physicist Oskar Klein gave a physical interpretation of the unobservable extra dimension—it is wrapped into a small circle. Einstein introduced a nonsymmetric metric tensor, while much later Brans and Dicke added a scalar component to gravity. These ideas would be revived within string theory, where they are demanded by consistency conditions.
String theory was originally developed during the late 1960s and early 1970s as a never completely successful theory of hadrons, the subatomic particles like the proton and neutron that feel the strong interaction. In the 1960s, Geoffrey Chew and Steven Frautschi discovered that the mesons make families called Regge trajectories with masses related to spins in a way that was later understood by Yoichiro Nambu, Holger Bech Nielsen and Leonard Susskind to be the relationship expected from rotating strings. Chew advocated making a theory for the interactions of these trajectories that did not presume that they were composed of any fundamental particles, but would construct their interactions from selfconsistency conditions on the Smatrix. The Smatrix approach was started by Werner Heisenberg in the 1940s as a way of constructing a theory that did not rely on the local notions of space and time, which Heisenberg believed break down at the nuclear scale. While the scale was off by many orders of magnitude, the approach he advocated was ideally suited for a theory of quantum gravity.
Working with experimental data, R. Dolen, D. Horn and C. Schmid^{[41]} developed some sum rules for hadron exchange. When a particle and antiparticle scatter, virtual particles can be exchanged in two qualitatively different ways. In the schannel, the two particles annihilate to make temporary intermediate states that fall apart into the final state particles. In the tchannel, the particles exchange intermediate states by emission and absorption. In field theory, the two contributions add together, one giving a continuous background contribution, the other giving peaks at certain energies. In the data, it was clear that the peaks were stealing from the background—the authors interpreted this as saying that the tchannel contribution was dual to the schannel one, meaning both described the whole amplitude and included the other.
The result was widely advertised by Murray GellMann, leading Gabriele Veneziano to construct a scattering amplitude that had the property of DolenHornSchmid duality, later renamed worldsheet duality. The amplitude needed poles where the particles appear, on straight line trajectories, and there is a special mathematical function whose poles are evenly spaced on half the real line— the Gamma function— which was widely used in Regge theory. By manipulating combinations of Gamma functions, Veneziano was able to find a consistent scattering amplitude with poles on straight lines, with mostly positive residues, which obeyed duality and had the appropriate Regge scaling at high energy. The amplitude could fit nearbeam scattering data as well as other Regge type fits, and had a suggestive integral representation that could be used for generalization.
Over the next years, hundreds of physicists worked to complete the bootstrap program for this model, with many surprises. Veneziano himself discovered that for the scattering amplitude to describe the scattering of a particle that appears in the theory, an obvious selfconsistency condition, the lightest particle must be a tachyon. Miguel Virasoro and Joel Shapiro found a different amplitude now understood to be that of closed strings, while Ziro Koba and Holger Nielsen generalized Veneziano's integral representation to multiparticle scattering. Veneziano and Sergio Fubini introduced an operator formalism for computing the scattering amplitudes that was a forerunner of worldsheet conformal theory, while Virasoro understood how to remove the poles with wrongsign residues using a constraint on the states. Claud Lovelace calculated a loop amplitude, and noted that there is an inconsistency unless the dimension of the theory is 26. Charles Thorn, Peter Goddard and Richard Brower went on to prove that there are no wrongsign propagating states in dimensions less than or equal to 26.
In 1969, Yoichiro Nambu, Holger Bech Nielsen, and Leonard Susskind recognized that the theory could be given a description in space and time in terms of strings. The scattering amplitudes were derived systematically from the action principle by Peter Goddard, Jeffrey Goldstone, Claudio Rebbi, and Charles Thorn, giving a spacetime picture to the vertex operators introduced by Veneziano and Fubini and a geometrical interpretation to the Virasoro conditions.
In 1970, Pierre Ramond added fermions to the model, which led him to formulate a twodimensional supersymmetry to cancel the wrongsign states. John Schwarz and André Neveu added another sector to the fermi theory a short time later. In the fermion theories, the critical dimension was 10. Stanley Mandelstam formulated a world sheet conformal theory for both the bose and fermi case, giving a twodimensional field theoretic pathintegral to generate the operator formalism. Michio Kaku and Keiji Kikkawa gave a different formulation of the bosonic string, as a string field theory, with infinitely many particle types and with fields taking values not on points, but on loops and curves.
In 1974, Tamiaki Yoneya discovered that all the known string theories included a massless spintwo particle that obeyed the correct Ward identities to be a graviton. John Schwarz and Joel Scherk came to the same conclusion and made the bold leap to suggest that string theory was a theory of gravity, not a theory of hadrons. They reintroduced Kaluza–Klein theory as a way of making sense of the extra dimensions. At the same time, quantum chromodynamics was recognized as the correct theory of hadrons, shifting the attention of physicists and apparently leaving the bootstrap program in the dustbin of history.
String theory eventually made it out of the dustbin, but for the following decade all work on the theory was completely ignored. Still, the theory continued to develop at a steady pace thanks to the work of a handful of devotees. Ferdinando Gliozzi, Joel Scherk, and David Olive realized in 1976 that the original Ramond and Neveu Schwarzstrings were separately inconsistent and needed to be combined. The resulting theory did not have a tachyon, and was proven to have spacetime supersymmetry by John Schwarz and Michael Green in 1981. The same year, Alexander Polyakov gave the theory a modern path integral formulation, and went on to develop conformal field theory extensively. In 1979, Daniel Friedan showed that the equations of motions of string theory, which are generalizations of the Einstein equations of General Relativity, emerge from the Renormalization group equations for the twodimensional field theory. Schwarz and Green discovered Tduality, and constructed two superstring theories—IIA and IIB related by Tduality, and type I theories with open strings. The consistency conditions had been so strong, that the entire theory was nearly uniquely determined, with only a few discrete choices.
First superstring revolution
In the early 1980s, Edward Witten discovered that most theories of quantum gravity could not accommodate chiral fermions like the neutrino. This led him, in collaboration with Luis AlvarezGaumé to study violations of the conservation laws in gravity theories with anomalies, concluding that type I string theories were inconsistent. Green and Schwarz discovered a contribution to the anomaly that Witten and AlvarezGaumé had missed, which restricted the gauge group of the type I string theory to be SO(32). In coming to understand this calculation, Edward Witten became convinced that string theory was truly a consistent theory of gravity, and he became a highprofile advocate. Following Witten's lead, between 1984 and 1986, hundreds of physicists started to work in this field, and this is sometimes called the first superstring revolution.
During this period, David Gross, Jeffrey Harvey, Emil Martinec, and Ryan Rohm discovered heterotic strings. The gauge group of these closed strings was two copies of E8, and either copy could easily and naturally include the standard model. Philip Candelas, Gary Horowitz, Andrew Strominger and Edward Witten found that the Calabi–Yau manifolds are the compactifications that preserve a realistic amount of supersymmetry, while Lance Dixon and others worked out the physical properties of orbifolds, distinctive geometrical singularities allowed in string theory. Cumrun Vafa generalized Tduality from circles to arbitrary manifolds, creating the mathematical field of mirror symmetry. Daniel Friedan, Emil Martinec and Stephen Shenker further developed the covariant quantization of the superstring using conformal field theory techniques. David Gross and Vipul Periwal discovered that string perturbation theory was divergent. Stephen Shenker showed it diverged much faster than in field theory suggesting that new nonperturbative objects were missing.
In the 1990s, Joseph Polchinski discovered that the theory requires higherdimensional objects, called Dbranes and identified these with the blackhole solutions of supergravity. These were understood to be the new objects suggested by the perturbative divergences, and they opened up a new field with rich mathematical structure. It quickly became clear that Dbranes and other pbranes, not just strings, formed the matter content of the string theories, and the physical interpretation of the strings and branes was revealed—they are a type of black hole. Leonard Susskind had incorporated the holographic principle of Gerardus 't Hooft into string theory, identifying the long highly excited string states with ordinary thermal black hole states. As suggested by 't Hooft, the fluctuations of the black hole horizon, the worldsheet or worldvolume theory, describes not only the degrees of freedom of the black hole, but all nearby objects too.
Second superstring revolution
In 1995, at the annual conference of string theorists at the University of Southern California (USC), Edward Witten gave a speech on string theory that in essence united the five string theories that existed at the time, and giving birth to a new 11dimensional theory called Mtheory. Mtheory was also foreshadowed in the work of Paul Townsend at approximately the same time. The flurry of activity that began at this time is sometimes called the second superstring revolution.
During this period, Tom Banks, Willy Fischler, Stephen Shenker and Leonard Susskind formulated matrix theory, a full holographic description of Mtheory using IIA D0 branes.^{[42]} This was the first definition of string theory that was fully nonperturbative and a concrete mathematical realization of the holographic principle. It is an example of a gaugegravity duality and is now understood to be a special case of the AdS/CFT correspondence. Andrew Strominger and Cumrun Vafa calculated the entropy of certain configurations of Dbranes and found agreement with the semiclassical answer for extreme charged black holes. Petr Hořava and Witten found the elevendimensional formulation of the heterotic string theories, showing that orbifolds solve the chirality problem. Witten noted that the effective description of the physics of Dbranes at low energies is by a supersymmetric gauge theory, and found geometrical interpretations of mathematical structures in gauge theory that he and Nathan Seiberg had earlier discovered in terms of the location of the branes.
In 1997, Juan Maldacena noted that the low energy excitations of a theory near a black hole consist of objects close to the horizon, which for extreme charged black holes looks like an antide Sitter space. He noted that in this limit the gauge theory describes the string excitations near the branes. So he hypothesized that string theory on a nearhorizon extremecharged blackhole geometry, an antideSitter space times a sphere with flux, is equally well described by the lowenergy limiting gauge theory, the N = 4 supersymmetric Yang–Mills theory. This hypothesis, which is called the AdS/CFT correspondence, was further developed by Steven Gubser, Igor Klebanov and Alexander Polyakov, and by Edward Witten, and it is now wellaccepted. It is a concrete realization of the holographic principle, which has farreaching implications for black holes, locality and information in physics, as well as the nature of the gravitational interaction. Through this relationship, string theory has been shown to be related to gauge theories like quantum chromodynamics and this has led to more quantitative understanding of the behavior of hadrons, bringing string theory back to its roots.
Criticisms
Some critics of string theory say that it is a failure as a theory of everything.^{[43]}^{[page needed]}^{[44]}^{[page needed]} Notable critics include Peter Woit,^{[45]}^{[46]} Lee Smolin, Philip Warren Anderson,^{[47]} Sheldon Glashow,^{[48]} Lawrence Krauss,^{[49]} Carlo Rovelli^{[50]} and Bert Schroer.^{[51]} Some common criticisms include:
 Very high energies needed to test quantum gravity.
 Lack of uniqueness of predictions due to the large number of solutions.
 Lack of manifest background independence.
High energies
It is widely believed that any theory of quantum gravity would require extremely high energies to probe directly, higher by orders of magnitude than those that current experiments such as the Large Hadron Collider^{[52]} can attain. This is because strings themselves are expected to be only slightly larger than the Planck length, which is twenty orders of magnitude smaller than the radius of a proton, and high energies are required to probe small length scales. Generally speaking, quantum gravity is difficult to test because gravity is much weaker than the other forces, and because quantum effects are controlled by Planck's constant h, a very small quantity. As a result, the effects of quantum gravity are extremely weak.
Number of solutions
String theory as it is currently understood has a huge number of solutions, called string vacua,^{[23]} and these vacua might be sufficiently diverse to accommodate almost any phenomena we might observe at lower energies.
The vacuum structure of the theory, called the string theory landscape (or the anthropic portion of string theory vacua), is not well understood. String theory contains an infinite number of distinct metastable vacua, and perhaps 10^{520} of these or more correspond to a universe roughly similar to ours—with four dimensions, a high planck scale, gauge groups, and chiral fermions. Each of these corresponds to a different possible universe, with a different collection of particles and forces.^{[23]} What principle, if any, can be used to select among these vacua is an open issue. While there are no continuous parameters in the theory, there is a very large set of possible universes, which may be radically different from each other. It is also suggested that the landscape is surrounded by an even more vast swampland of consistentlooking semiclassical effective field theories, which are actually inconsistent.^{[53]}
Some physicists believe this is a good thing, because it may allow a natural anthropic explanation of the observed values of physical constants, in particular the small value of the cosmological constant.^{[54]}^{[55]} The argument is that most universes contain values for physical constants that do not lead to habitable universes (at least for humans), and so we happen to live in the "friendliest" universe. This principle is already employed to explain the existence of life on Earth as the result of a lifefriendly orbit around the mediumsized sun among an infinite number of possible orbits (as well as a relatively stable location in the galaxy).
Background independence
A separate and older criticism of string theory is that it is not manifestly backgroundindependent — string theory describes perturbative expansions about fixed spacetime backgrounds which means that mathematical calculations in the theory rely on preselecting a background as a starting point. This is because, like many quantum field theories, much of string theory is still only formulated perturbatively, as a divergent series of approximations.^{[citation needed]}
Although the theory, defined as a perturbative expansion on a fixed background, is not background independent, it has some features that suggest nonperturbative approaches would be backgroundindependent—topology change is an established process in string theory, and the exchange of gravitons is equivalent to a change in the background. Since there are dynamic corrections to the background spacetime in the perturbative theory, one would expect spacetime to be dynamic in the nonperturbative theory as well since they would have to predict the same spacetime.^{[citation needed]}
This criticism has been addressed to some extent by the AdS/CFT duality, which is believed to provide a full, nonperturbative definition of string theory in spacetimes with antide Sitter space asymptotics. Nevertheless, a nonperturbative definition of the theory in arbitrary spacetime backgrounds is still lacking. Some hope that Mtheory, or a nonperturbative treatment of string theory (such as "background independent open string field theory") will have a backgroundindependent formulation.^{[citation needed]}
See also
 Conformal field theory
 Glossary of string theory
 List of string theory topics
 Loop quantum gravity
 Supergravity
 Supersymmetry
References
 ↑ Sean Carroll, Ph.D., Caltech, 2007, The Teaching Company, Dark Matter, Dark Energy: The Dark Side of the Universe, Guidebook Part 2 page 59, Accessed Oct. 7, 2013, "...The idea that the elementary constituents of matter are small loops of string rather than pointlike particles ... we think of string theory as a candidate theory of quantum gravity..."
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ String theory  a very brief history
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ P.C.W. Davies and J. Brown (ed), Superstrings, A Theory of Everything?, Cambridge University Press, 1988 (ISBN 0521357411).
 ↑ Penrose, Roger (2005). The Road to Reality: A Complete Guide to the Laws of the Universe. Knopf. ISBN 0679454438.
 ↑ Sheldon Glashow. "NOVA – The elegant Universe". Pbs.org. Retrieved on 20120711.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Duality in string theory in nLab
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Polchinski, Joseph (1998). String Theory, Cambridge University Press ISBN 0521672295.
 ↑ The calculation of the number of dimensions can be circumvented by adding a degree of freedom, which compensates for the "missing" quantum fluctuations. However, this degree of freedom behaves similar to spacetime dimensions only in some aspects, and the produced theory is not Lorentz invariant, and has other characteristics that do not appear in nature. This is known as the linear dilaton or noncritical string.
 ↑ Botelho, Luiz C. L. and Botelho, Raimundo C. L. (1999) "Quantum Geometry of Bosonic Strings – Revisited". Centro Brasileiro de Pesquisas Físicas.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ ^{23.0} ^{23.1} ^{23.2} Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Maldacena, J. The Large N Limit of Superconformal Field Theories and Supergravity, arXiv:hepth/9711200
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ 6d (2,0)supersymmetric QFT in nLab
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.^{[dead link]}
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ ^{40.0} ^{40.1} Suomalaistutkija kilpaili Einsteinin kanssa ja keksi viidennen ulottuvuuden  Tiede  Tiede  Helsingin Sanomat
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Woit, Peter Not Even Wrong. Math.columbia.edu. Retrieved on 20120711.
 ↑ Smolin, Lee. The Trouble With Physics. Thetroublewithphysics.com. Retrieved on 20120711.
 ↑ Woit, P. (Columbia University), String theory: An Evaluation, February 2001, arXiv:physics/0102051
 ↑ Woit, P. Is String Theory Testable? INFN Rome March 2007
 ↑ God (or Not), Physics and, of Course, Love: Scientists Take a Leap, New York Times, 4 January 2005: "String theory is the first science in hundreds of years to be pursued in preBaconian fashion, without any adequate experimental guidance"
 ↑ "there ain't no experiment that could be done nor is there any observation that could be made that would say, `You guys are wrong.' The theory is safe, permanently safe" NOVA interview
 ↑ Krauss, Lawrence (8 November 2005) Science and Religion Share Fascination in Things Unseen. New York Times: "String theory [is] yet to have any real successes in explaining or predicting anything measurable".
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ Schroer, B. (2008) String theory and the crisis of particle physics II or the ascent of metaphoric arguments, arXiv:0805.1911
 ↑ Kiritsis, Elias (2007) String Theory in a Nutshell, Princeton University Press, ISBN 1400839335.
 ↑ Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 ↑ ArkaniHamed, N.; Dimopoulos, S. and Kachru, S. Predictive Landscapes and New Physics at a TeV, arXiv:hepth/0501082, SLACPUB10928, HUTP05A0001, SUITP0444, January 2005
 ↑ Susskind, L. The Anthropic Landscape of String Theory, arXiv:hepth/0302219, February 2003
Further reading
Popular books
General
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
Critical
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
Textbooks
For physicists
 Becker, Katrin, Becker, Melanie, and Schwarz, John (2007) String Theory and MTheory: A Modern Introduction . Cambridge University Press. ISBN 0521860695
 Dine, Michael (2007) Supersymmetry and String Theory: Beyond the Standard Model. Cambridge University Press. ISBN 0521858410.
 Kiritsis, Elias (2007) String Theory in a Nutshell. Princeton University Press. ISBN 9780691122304.
 Michael Green, John H. Schwarz and Edward Witten (1987) Superstring theory. Cambridge University Press.
 Vol. 1: Introduction. ISBN 0521357527.
 Vol. 2: Loop amplitudes, anomalies and phenomenology. ISBN 0521357535.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Polchinski, Joseph (1998) String theory. Cambridge University Press.
 Vol. 1: An Introduction to the Bosonic String. ISBN 0521633036.
 Vol. 2: Superstring Theory and Beyond. ISBN 0521633044.
 Szabo, Richard J. (2007) An Introduction to String Theory and Dbrane Dynamics. Imperial College Press. ISBN 9781860944277.
 Zwiebach, Barton (2004) A First Course in String Theory. Cambridge University Press. ISBN 0521831431.
For mathematicians
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.^{[dead link]}
Online material
 Klebanov, Igor and Maldacena, Juan (January 2009). "Solving Quantum Field Theories via Curved Spacetimes". Physics Today.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.^{[dead link]}
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
 Lua error in Module:Citation/CS1 at line 746: Argument map not defined for this variable.
External links
Look up string theory in Wiktionary, the free dictionary. 
Error creating thumbnail: File missing 
PhysicsWiki Commons has media related to String theory. 
 Why String Theory—An introduction to string theory.
 Dialogue on the Foundations of String Theory at MathPages
 Superstrings! String Theory Home Page—Online tutorial
 A Layman’s Guide to String Theory—An explanation for the layperson
 Not Even Wrong—A blog critical of string theory
 The Official String Theory Web Site
 The Elegant Universe—A threehour miniseries with Brian Greene by NOVA (original PBS Broadcast Dates: October 28, 8–10 p.m. and November 4, 8–9 p.m., 2003). Various images, texts, videos and animations explaining string theory.
 Beyond String Theory—A project by a string physicist explaining aspects of string theory to a broad audience
 "String Theory" on YouTube
 Articles with dead external links from March 2015
 PhysicsWiki articles needing clarification from August 2014
 PhysicsWiki articles needing page number citations from April 2015
 String theory
 Concepts in physics
 Dimension
 Multidimensional geometry
 Particle physics
 Physical cosmology
 Physics beyond the Standard Model
 Theoretical physics