String theory
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String theory  
Superstring theory


String theory is a developing branch of theoretical physics that combines quantum mechanics and general relativity into a quantum theory of gravity. The strings of string theory are onedimensional oscillating lines, but they are no longer considered fundamental to the theory, which can be formulated in terms of points or surfaces too.
Since its birth as the dual resonance model which described the strongly interacting hadrons as strings, the term string theory has changed to include any of a group of related superstring theories which unite them. One shared property of all these theories is the holographic principle. String theory itself comes in many different formulations, each one with a different mathematical structure, and each best describing different physical circumstances. But the principles shared by these approaches, their mutual logical consistency, and the fact that some of them easily include the standard model of particle physics, has led many physicists to believe that the theory is the correct fundamental description of nature. In particular, string theory is the first candidate for the theory of everything, a way to describe all the known natural forces (gravitational, electromagnetic, weak and strong interactions) and matter (quarks and leptons) in a mathematically complete system.
Many detractors criticise string theory because it has not yet provided quantitative experimental predictions. Like any other quantum theory of gravity, it is widely believed that testing the theory directly by experiment would require prohibitively expensive feats of engineering. Whether there are stringent indirect tests of the theory is not yet known.
String theory is of interest to many physicists because it requires new mathematical and physical ideas to mesh together its very different mathematical formulations. One of the most inclusive of these is the 11dimensional Mtheory, and in the Mtheory way of thinking, string theory requires spacetime to have eleven dimensions,^{[1]} as opposed to the usual three space and one 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 not described by a real number, but by completely different type of mathematical quantity. So the notion of spacetime dimension is not a fixed thing in string theory: it is best thought of as different in different circumstances.^{[2]}
String theories include objects more general than strings, called branes. The word brane, derived from "membrane", refers to a variety of interrelated objects, such as Dbranes, black pbranes and NeveuSchwarz 5branes. These are extended objects that are charged sources for differential form generalizations of the vector potential electromagnetic field. These objects are related to oneanother by a variety of dualities. Black holelike black pbranes are identified with Dbranes, which are endpoints for strings, and this identification is called Gaugegravity duality. Research on this equivalence has led to new insights on quantum chromodynamics, the fundamental theory of the strong nuclear force.^{[3]}^{[4]}^{[5]}^{[6]}
Contents 
[edit] Overview
In string theory the electrons and quarks inside an atom are not 0dimensional objects, but 1dimensional strings. These strings can move and vibrate, giving the observed particles their flavor, charge, mass and spin. The strings make closed loops unless they encounter surfaces, called Dbranes, where they can open up into one dimensional lines. The endpoints of the string can't break off the Dbrane, but they can slide around on it.
String theory is a theory of gravity, an extension of General Relativity, and the classical interpretation of the strings and branes is that they are quantum mechanical vibrating extended charged black holes. The overarching physical insight behind string theory is the holographic principle, which states that the description of the oscillations of the surface of a black hole must also describe the spacetime around it. Holography demands that a lowdimensional theory describing the fluctuations of a horizon will end up describing everything that can fall through, which can be anything at all. So a theory of a black hole horizon is a theory of everything.
Finding even one consistent holographic description, a priori, seems like a longshot, because it would be a disembodied nonlocal description of quantum gravity. In string theory, not only is there one such description, there are several different ones, each describing fluctuations of horizons with different charges and dimensions, and all of them logically fit together. So the same physical objects and interactions can be described by the fluctuations of onedimensional black hole horizons, or by threedimensional horizons, or by zerodimensional horizons. The fact that these different descriptions describe the same physics is evidence that string theory is consistent.
An ordinary astronomical black hole does not have a convenient holographic description, because it has a Hawking temperature. String theories are formulated on cold black holes, which are those which have as much charge as possible. The first holographic theory discovered described the scattering of onedimensional strings, tiny loops of vibrating horizon charged with a twoform vector potential which makes a charged black hole a onedimensional line. Fluctuations of this line horizon describe all matter, so every elementary particle can be described by a mode of oscillation of a very small segment or loop of string. The stringlength is approximately the Planck length, but can be significantly bigger when the strings are weakly interacting.
All string theories predict the existence of degrees of freedom which are usually described as extra dimensions. Without fermions, bosonic strings can vibrate in a flat but unstable 26dimensional space time. In a superstring theory with fermions, the weakcoupling (nointeraction) limit describes a flat stable 10dimensional space time. Interacting superstring theories are best thought of as configurations of an 11 dimensional supergravity theory called Mtheory where one or more of the dimensions are curled up so that the lineextended charged black holes become long and light.
Long light strings can vibrate at different resonant frequencies, and each resonant frequency describes a different type of particle.^{[7]} So in string limits, any elementary particle should be thought of as a tiny vibrating line, rather than as a point. The string can vibrate in different modes just as a guitar string can produce different notes, and every mode appears as a different particle: electron, photon, gluon, etc.
The only way in which strings can interact is by splitting and combining in a smooth way. It is impossible to introduce arbitrary extra matter, like point particles which interact with strings by collisions, because the particles can fall into the black hole, so holography demands that it must show up as a mode of oscillation. The only way to introduce new matter is to find gravitational backgrounds where strings can scatter consistently, or to add boundary conditions, endpoints for the strings. Some of the backgrounds are called NSbranes, which are extremecharged black hole sheets of different dimensions. Other charged blacksheet backgrounds are the Dbranes, which have an alternate description as planes where strings can end and slide. When the strings are long and light, the branes are classical and heavy. In other limits where the strings become heavy, some of the branes can become light.
Since string theory is widely believed to be a consistent theory of quantum gravity, many hope that it correctly describes our universe, making it a theory of everything. There are known configurations which describe all the observed fundamental forces and matter but with a zero cosmological constant and some new fields. There are other configurations with different values of the cosmological constant, which are metastable but longlived. This leads many to believe that there is at least one metastable solution which is quantitatively identical with the standard model, with a small cosmological constant, which contains dark matter and a plausible mechanism for inflation. It is not yet known whether string theory has such a solution, nor how much freedom the theory allows to choose the details. Because of this, string theory has not yet made practically falsifiable predictions that would allow it to be experimentally tested.
The full theory does not yet have a satisfactory definition in all circumstances, since the scattering of strings is most straightforwardly defined by a perturbation theory. The complete quantum mechanics of high dimensional branes is not easily defined, and the behavior of string theory in cosmological settings (timedependent backgrounds) is not fully worked out. It is also not clear if there is any principle by which string theory selects its vacuum state, the spacetime configuration which determines the properties of our Universe (see string theory landscape).
[edit] Basic properties
String theory can be formulated in terms of an action principle, either the NambuGoto action or the Polyakov action, which describes how strings move through space and time. In the absence of external interactions, string dynamics are governed by tension and kinetic energy, which combine to produce oscillations. The quantum mechanics of strings implies these oscillations take on discrete vibrational modes, the spectrum of the theory.
On distance scales larger than the string radius, each oscillation mode behaves as a different species of particle, with its mass, spin and charge determined by the strings dynamics. Splitting and recombinations of string 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 but distinct musical notes. In the analogy, different notes correspond to different particles. The only difference is the guitar is only 2dimensional, you can strum it up, and down. In actuality the guitar strings would be every dimension, and the strings could vibrate in any direction. Meaning that the particles could move through not only our dimension, but other dimensions as well.
String theory includes both open strings, which have two distinct endpoints, and closed strings making a complete loop. The two types of string behave in slightly different ways, yielding two different spectra. For example, in most string theories, one of the closed string modes is the graviton, and one of the open string modes is the photon. Because the two ends of an open string can always meet and connect, forming a closed string, there are no string theories without closed strings.
The earliest string model, the bosonic string, incorporated only bosons. This model describes, in low enough energies, a quantum gravity theory, which also includes (if open strings are incorporated as well) gauge fields such as the photon (or, more generally, any gauge theory). However, this model has problems. Most importantly, the theory has a fundamental instability, believed to result in the decay (at least partially) of spacetime itself. Additionally, 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 in its spectrum led to the invention of supersymmetry, a mathematical relation between bosons and fermions. String theories which include fermionic vibrations are now known as superstring theories; several different kinds have been described, but all are now thought to be different limits of Mtheory.
Some qualitative properties of quantum strings can be understood in a fairly simple fashion. For example, quantum strings have tension, much like regular strings made of twine; this tension is considered a fundamental parameter of the theory. The tension of a quantum string is closely related to its size. Consider a closed loop of string, left to move through space without external forces. Its tension will tend to contract it into a smaller and smaller loop. Classical intuition suggests that it might shrink to a single point, but this would violate Heisenberg's uncertainty principle. The characteristic size of the string loop will be a balance between the tension force, acting to make it small, and the uncertainty effect, which keeps it "stretched". Consequently, the minimum size of a string is related to the string tension.
[edit] Worldsheet
A pointlike particle's motion may be described by drawing a graph of its position (in one or two dimensions of space) against time. The resulting picture depicts the worldline of the particle (its 'history') in spacetime. By analogy, a similar graph depicting the progress of a string as time passes by can be obtained; the string (a onedimensional object — a small line — by itself) will trace out a surface (a twodimensional manifold), known as the worldsheet. The different string modes (representing different particles, such as photon or graviton) are surface waves on this manifold.
A closed string looks like a small loop, so its worldsheet will look like a pipe or, more generally, a Riemannian surface (a twodimensional oriented manifold) with no boundaries (i.e. no edge). An open string looks like a short line, so its worldsheet will look like a strip or, more generally, a Riemann surface with a boundary.
Strings can split and connect. This is reflected by the form of their worldsheet (more accurately, by its topology). For example, if a closed string splits, its worldsheet will look like a single pipe splitting (or connected) to two pipes (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 ingoing string, and the other — the outgoing one). An open string doing the same thing will have its worldsheet looking like a ring connected to two strips.
Note that the process of a string splitting (or strings connecting) is a global process of the worldsheet, not a local one: locally, the worldsheet looks the same everywhere and it is not possible to determine a single point on the worldsheet where the splitting occurs. Therefore these processes are an integral part of the theory, and are described by the same dynamics that controls the string modes.
In some string theories (namely, closed strings in Type I and some versions of the bosonic string), strings can split and reconnect in an opposite orientation (as in a Möbius strip or a Klein bottle). These theories are called unoriented. Formally, the worldsheet in these theories is a nonorientable surface.
[edit] Dualities
Before the 1990s, string theorists believed there were five distinct superstring theories: open type I, closed type I, closed type IIA, closed type IIB, and the two flavors of heterotic string theory (SO(32) and E_{8}×E_{8})^{[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 connected to one another as if they are each a special case of some more fundamental theory (thought to be Mtheory). These theories are related by transformations that are called dualities. If two theories are related by a duality transformation, it means that the first theory can be transformed in some way so that it ends up looking just like the second theory. The two theories are then said to be dual to one another under that kind of transformation. Put differently, the two theories are mathematically different descriptions of the same phenomena.
These dualities link quantities that were also thought to be separate. 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 field theory and quantum particle 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.
Before the "duality revolution" there were believed to be five distinct versions of string theory, plus the (unstable) bosonic and gluonic theories.
String theories  

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; group symmetry is SO(32) 
IIA  10  Supersymmetry between forces and matter, with closed strings and open strings bound to Dbranes; no tachyon; massless fermions are nonchiral 
IIB  10  Supersymmetry between forces and matter, with closed strings and open strings bound to Dbranes; 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; group symmetry is SO(32) 
HE  10  Supersymmetry between forces and matter, with closed strings only; no tachyon; heterotic, meaning right moving and left moving strings differ; group symmetry is E_{8}×E_{8} 
Note that in the type IIA and type IIB string theories closed strings are allowed to move everywhere throughout the tendimensional spacetime (called the bulk), while open strings have their ends attached to Dbranes, which are membranes of lower dimensionality (their dimension is odd — 1, 3, 5, 7 or 9 — in type IIA and even — 0, 2, 4, 6 or 8 — in type IIB, including the time direction).
[edit] Extra dimensions
[edit] Number of dimensions
An intriguing feature of string theory is that it involves the prediction of extra dimensions. The number of dimensions is not fixed by any consistency criterion, but flat spacetime solutions do exist in the socalled "critical dimension". Cosmological solutions exist in a wider variety of dimensionalities, and these different dimensions—more precisely different values of the "effective central charge", a count of degrees of freedom which reduces to dimensionality in weakly curved regimes—are related by dynamical transitions.^{[9]}
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 "by hand", and this number is fixed and independent of potential energy. String theory allows one to relate the number of dimensions to scalar potential energy. Technically, 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 which is predicted by string theory depends on the energy of the string mode which 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.^{[10]}
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 fluxuations 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.^{[11]} Starting from any dimension greater than four, it is necessary to consider how these are reduced to four dimensional spacetime.
[edit] Compact dimensions
Two different 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 present day 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 CalabiYau 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 CalabiYau or G2 manifolds.
A standard analogy for this is to consider multidimensional space as a garden hose. If the hose is viewed from a 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 waveparticle duality).
[edit] Braneworld scenario
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Another possibility is that we are "stuck" in a 3+1 dimensional (i.e. three spatial dimensions plus the time dimension) subspace of the full universe. This subspace is supposed to be a Dbrane, hence this is known as a braneworld theory. Some believe that some combination of the two ideas — compactification and branes — will ultimately yield the most realistic theory.^{[citation needed]}
[edit] Effect of the hidden dimensions
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 CalabiYau 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.
[edit] Dbranes
Another key feature of string theory is the existence of Dbranes. These are membranes of different dimensionality (anywhere from a zero dimensional membrane — which is in fact a point — and up, including 2dimensional membranes, 3dimensional volumes and so on).
Dbranes are defined by the fact that worldsheet boundaries are attached to them. Thus Dbranes can emit and absorb closed strings; therefore they have mass (since they emit gravitons) and — in superstring theories — charge as well (since they emit closed strings which are gauge bosons).
From the point of view of open strings, Dbranes are objects to which the ends of open strings are attached. The open strings attached to a Dbrane are said to "live" on it, and they give rise to gauge theories "living" on it (since one of the open string modes is a gauge boson such as the photon). In the case of one Dbrane there will be one type of a gauge boson and we will have an Abelian gauge theory (with the gauge boson being the photon). If there are multiple parallel Dbranes there will be multiple types of gauge bosons, giving rise to a nonAbelian gauge theory.
Dbranes are thus gravitational sources, on which a gauge theory "lives". This gauge theory is coupled to gravity (which is said to exist in the bulk), so that normally each of these two different viewpoints is incomplete.
[edit] Gaugegravity duality
Gaugegravity duality is a conjectured duality between a quantum theory of gravity in certain cases and gauge theory in a lower number of dimensions. This means that each predicted phenomenon and quantity in one theory has an analogue in the other theory, with a "dictionary" translating from one theory to the other.
[edit] Description of the duality
In certain cases the gauge theory on the Dbranes is decoupled from the gravity living in the bulk; thus open strings attached to the Dbranes are not interacting with closed strings. Such a situation is termed a decoupling limit.
In those cases, the Dbranes have two independent alternative descriptions. As discussed above, from the point of view of closed strings, the Dbranes are gravitational sources, and thus we have a gravitational theory on spacetime with some background fields. From the point of view of open strings, the physics of the Dbranes is described by the appropriate gauge theory. Therefore in such cases it is often conjectured that the gravitational theory on spacetime with the appropriate background fields is dual (i.e. physically equivalent) to the gauge theory on the boundary of this spacetime (since the subspace filled by the Dbranes is the boundary of this spacetime). So far, this duality has not been proven in any cases, so there is also disagreement among string theorists regarding how strong the duality applies to various models.
[edit] Examples and intuition
The most wellknown example and the first one to be studied is the duality between Type IIB supergravity on AdS^{5} S^{5} (a product space of a fivedimensional Anti de Sitter space and a fivesphere) on one hand, and N = 4 supersymmetric YangMills theory on the fourdimensional boundary of the Anti de Sitter space (either a flat fourdimensional spacetime R^{3,1} or a threesphere with time S^{3} R).^{[12]} This is known as the AdS/CFT correspondence, a name often used for Gauge / gravity duality in general.
This duality can be thought of as follows: suppose there is a spacetime with a gravitational source, for example an extremal black hole. When particles are far away from this source, they are described by closed strings (i.e. a gravitational theory, or usually supergravity). As the particles approach the gravitational source, they can still be described by closed strings; alternatively, they can be described by objects similar to QCD strings, which are made of gauge bosons (gluons) and other gauge theory degrees of freedom. So if one is able (in a decoupling limit) to describe the gravitational system as two separate regions — one (the bulk) far away from the source, and the other close to the source — then the latter region can also be described by a gauge theory on Dbranes. This latter region (close to the source) is termed the nearhorizon limit, since usually there is an event horizon around (or at) the gravitational source.
In the gravitational theory, one of the directions in spacetime is the radial direction, going from the gravitational source and away (towards the bulk). The gauge theory lives only on the Dbrane itself, so it does not include the radial direction: it lives in a spacetime with one less dimension compared to the gravitational theory (in fact, it lives on a spacetime identical to the boundary of the nearhorizon gravitational theory). Let us understand how the two theories are still equivalent:
The physics of the nearhorizon gravitational theory involves only onshell states (as usual in string theory), while the field theory includes also offshell correlation function. The onshell states in the nearhorizon gravitational theory can be thought of as describing only particles arriving from the bulk to the nearhorizon region and interacting there between themselves. In the gauge theory these are "projected" onto the boundary, so that particles which arrive at the source from different directions will be seen in the gauge theory as (offshell) quantum fluctuations far apart from each other, while particles arriving at the source from almost the same direction in space will be seen in the gauge theory as (offshell) quantum fluctuations close to each other. Thus the angle between the arriving particles in the gravitational theory translates to the distance scale between quantum fluctuations in the gauge theory. The angle between arriving particles in the gravitational theory is related to the radial distance from the gravitational source at which the particles interact: the larger the angle, the closer the particles have to get to the source in order to interact with each other. On the other hand, the scale of the distance between quantum fluctuations in a quantum field theory is related (inversely) to the energy scale in this theory. So small radius in the gravitational theory translates to low energy scale in the gauge theory (i.e. the IR regime of the field theory) while large radius in the gravitational theory translates to high energy scale in the gauge theory (i.e. the UV regime of the field theory).
A simple example to this principle is that if in the gravitational theory there is a setup in which the dilaton field (which determines the strength of the coupling) is decreasing with the radius, then its dual field theory will be asymptotically free, i.e. its coupling will grow weaker in high energies.
[edit] Contact with experiment
This branch of string theory may lead to new insights on quantum chromodynamics, a gauge theory which is the fundamental theory of the strong nuclear force. To this end, it is hoped that a gravitational theory dual to quantum chromodynamics will be found.^{[13]}
In fact, a vague contact with experiment has already been claimed to have been achieved^{[3]}^{[4]}^{[5]}^{[6]}, though currently the alternative explanation for quarkgluon plasma behavior, Lattice QCD, is doing a much better job and has already made contact with experiments in various fields with good results,^{[14]} though the computations are numerical rather than analytic. Other possible experiments for string theory have been proposed. One is the discovery of large cosmic strings in space, formed when the high energies in the Big Bang "stretched" some strings to astronomical proportions. Other possible avenues of experiment which could help provide evidence for string theory may take place at the newly built Large Hadron Collider. One is the measurement of the strength of gravity on a microscopic scale, which could provide evidence for extra dimensions; if gravitons (which are closed strings) leak off the membrane, at small scales the force of gravity should be much greater than at large scales where the gravitons would have ample chance to leak away into the bulk. The discovery of supersymmetry could also be considered evidence since string theory was the first theory to require it, though other theories have managed to incorporate supersymmetry as well. Also, the absence of supersymmetric particles at energies accessible to the LHC would not necessarily disprove string theory, since supersymmetry could exist but still be outside the accelerator's range.
[edit] Problems and controversy
Although string theory is an outgrowth of physics, some contend that string theory's current untestable status means that it should be classified as more of a mathematical framework for building models as opposed to a physical theory^{[15]}. For a theory to be physics, it must be corroborated empirically, through experiment or observation, but few avenues for such contact with experiment have been claimed.^{[16]}
[edit] Is string theory falsifiable?
Following the appearance of two books claiming string theory has failed,^{[17]}^{[18]} a hot media debate evolved in 2007.^{[19]}^{[20]}
 "For more than a generation, physicists have been chasing a willo’thewisp called string theory. The beginning of this chase marked the end of what had been threequarters of a century of progress. Dozens of stringtheory conferences have been held, hundreds of new Ph.D.s have been minted, and thousands of papers have been written. Yet, for all this activity, not a single new testable prediction has been made, not a single theoretical puzzle has been solved. In fact, there is no theory so far—just a set of hunches and calculations suggesting that a theory might exist. And, even if it does, this theory will come in such a bewildering number of versions that it will be of no practical use: a Theory of Nothing."^{[21]}  Jim Holt
The controversy centers around two properties of string theory:
 It is widely believed that any theory of quantum gravity would require extremely high energies to probe directly, higher by orders of magnitude than current experiments such as the Large Hadron Collider^{[22]}.
 String theory as it is currently understood has a huge number of equally possible solutions, called string vacua^{[23]} and some scientists believe that these vacua are sufficiently diverse to explain anything.
If these properties are both true, string theory as a theory of everything has no predictive power for low energy experiments, and would probably not be falsifiable by any current or future experiments.^{[17]}^{[24]}^{[25]}^{[18]} Because the theory is so difficult to test in the foreseeable future, some theoretical physicists^{[26]} have asked if it can be called a scientific theory, as it is not yet definitively Popper falsifiable.
String theory does predict, at least perturbatively, that at sufficiently high energies—which are probably near the quantum gravity scale—the stringlike nature of particles should be apparent. For example, there should be heavier copies of all particles corresponding to higher string harmonics. However, it is unclear how high these energies are. In the most likely case, these energies would be 10^{15} times higher than those accessible in the newest particle accelerator, the LHC. This would make it very difficult to probe string theory directly.
[edit] Swampland
In response to these concerns, Cumrun Vafa and others have challenged the idea that string theory is compatible with anything. They propose that most possible theories of low energy physics lie in the swampland. The swampland is the collection of theories which could be true if gravity wasn't an issue, but which are not compatible with string theory. An example of a theory in the swampland is quantum electrodynamics in the limit of very small electron charge. This limit is perfectly fine in quantum field theory in fact, in this limit, the perturbation theory becomes better and better. But in string theory, at the moment the charge of the lightest charged particle becomes less than the mass in natural units, the theory becomes inconsistent.
The reason is that two such charged massive particles will attract each other gravitationally more than they repel each other electrostatically, and could be used to form black holes. If there are no light charged particles, these black holes could not decay efficiently, barring improbable conspiracies or remnants. From the study of examples, and from the analysis of blackhole evaporation, it is now accepted that theories with a small charge quantum must come with light charged particles. This is only true within string theory  there is no such restriction in quantum field theory. This means that the discovery of a new gauge group with a small quantum of charge and only heavy charged particles would falsify string theory. Since this argument is very general  relying only on blackhole evaporation and the holographic principle, it has been suggested that this prediction would be true of any consistent holographic theory of quantum gravity, although the phrase "consistent holographic theory of quantum gravity" might very well be synonymous with "string theory".
It is notable that all the gross feature of the Standard model can be embedded within String theory, so that the standard model is not in the swampland. This includes features such as nonabelian gauge groups and chiral fermions which are hard to incorporate in nonstring theories of quantum gravity.
[edit] Background independence
A separate and older criticism of string theory is that it is backgrounddependent — string theory describes perturbative expansions about fixed spacetime backgrounds. Although the theory has some backgroundindependence — topology change is an established process in string theory, and the exchange of gravitons is equivalent to a change in the background — mathematical calculations in the theory relies 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. Although nonperturbative techniques have progressed considerably — including conjectured complete definitions in spacetimes satisfying certain asymptotics — a full nonperturbative definition of the theory is still lacking. Some see background independence as a fundamental requirement of a theory of quantum gravity, particularly since General Relativity is already background independent. Some hope that Mtheory, or a nonperturbative treatment of string theory (string field theory was thought to be nonperturbative in the 1980s) have a backgroundindependent formulation.
[edit] SUSY (Supersymmetry) breaking
A central problem for applications is that the best understood backgrounds of string theory preserve much of the supersymmetry of the underlying theory, which results in timeinvariant spacetimes: currently string theory cannot deal well with timedependent, cosmological backgrounds. However, several models have been proposed to explain supersymmetry breaking, most notably the KKLT model^{[23]}, which incorporates branes and fluxes to make a metastable compactification.
The vacuum structure of the theory, called the string theory landscape, is not well understood. String theory contains an infinite number of distinct metastable vacua, and perhaps 10^{500} 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.
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.^{[27]}^{[28]} The argument is that most universes contain values for physical constants which lead to inhabitable universes (at least for humans), and we happen to live in the most "friendly" 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). However, the cosmological version of the anthropic principle remains highly controversial because it would be difficult if not impossible to Popper falsify; so many do not accept it as scientific.
[edit] Other testability criteria
Many physicists strongly oppose the idea that string theory is not falsifiable, among them Sylvester James Gates: "So, the next time someone tells you that string theory is not testable, remind them of the AdS/CFT connection ..."^{[29]}. AdS/CFT relates string theory to gauge theory, and allows contact with low energy experiments in quantum chromodynamics. This type of string theory, which only describes the strong interactions, is much less controversial today than string theories of everything^{[30]}
In addition, Gates points out that the grand unification natural in string theories of everything requires that the coupling constants of the four forces meet at one point under renormalization group rescaling. This is also a falsifiable statement, but it is not restricted to string theory, but is shared by grand unified theories.^{[31]}. The LHC will be used both for testing AdS/CFT, and to check if the electroweakstrong unification does happen as predicted.^{[32]}.
[edit] History
It has been suggested that this section be split into a new article. (Discuss) 
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 general relativity was German mathematician Theodor Kaluza in 1919, who noted that gravity in five dimensions describes both gravity and electromagnetism in four. 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 geometric 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 which 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 and Leonard Susskind to be the relationship expected from rotating strings. Chew advocated making a theory for the interactions of these trajectories which 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 which 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. Schmidt 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 which 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 which had the property of DolenHornSchmidt 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 which 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 which 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 which 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 which 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 KaluzaKlein 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 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 different 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.
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 CalabiYau manifolds are the compactifications which 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. David Gross and Vipul Periwal discovered that string perturbation theory was divergent in a way that suggested 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 highlyexcited 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.
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 essentially 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 which began at this time is sometimes called the second superstring revolution.
During this period, Tom Banks, Willy Fischler Stephen Shenker and Leonard Susskind formulated a full holographic description of Mtheory on IIA D0 branes, the first definition of string theory that was fully nonperturbative and a concrete mathematical realization of the holographic principle. 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 Horava and Edward 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 anti de 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 YangMills theory. This hypothesis, complemented by converging work due to Steven Gubser, Igor Klebanov and Alexander Polyakov, is called the AdS/CFT correspondence 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.
[edit] Popular culture
 The book The Elegant Universe by Brian Greene, Professor of Physics at Columbia University, was adapted into a threehour documentary for Nova and also shown on British television. It was also shown by Discovery Channel on Indian television, as well as in Australia on SBS and in Argentina in the channel Encuentro.
 String Theory is also a trilogy of novels based on the Star Trek: Voyager television series.
 The CalabiYau space is mentioned in reference to a hypothetical matter quantum teleportation (QT for short) in the novels Ilium and Olympos, by Science Fiction writer Dan Simmons. In addition, several other hypothetical quantummechanics and string theoryrelated concepts are employed and to some extent explained or described in the books: Brane holes, parallel universes, singularities (black holes and wormholes), "quantum" morphing/shapeshifting devices and the intrinsic probabilistic nature of the quantum mechanical theory.
 Tool (band) references the String Theory in the beginning of their song Third Eye (song).
 In "H. P. Lovecraft's Dreams in the WitchHouse", an episode of the Showtime series Masters of Horror (based on a story by H. P. Lovecraft and directed by Stuart Gordon), a young grad student from Miskatonic University studies interdimensional string theory in his rundown apartment and discovers the intersection of two separate realities.
 String theory and its related philosophy features prominently in River of Gods, a sciencefiction novel by Ian McDonald set in futuristic India.
 On "The Big Bang Theory", Sheldon's major research is in string theory.
 Lupe Fiasco mentions the string theory in his song "Hurt Me Soul".
 String Theory was a major reference and title in the CSI episode titled "The Theory of Everything".
 In the episode The Suite Smell of Excess on Disney's The Suite Life Of Zack And Cody, Arwin invents a P.U., a device that can transport people from one universe to a parallel one, which works on the properties of String Theory.
 String Theory is constantly referenced comically in Zippy comic strips, by Bill Griffith.
[edit] See also
 AdS/CFT correspondence
 Conformal field theory
 Dual resonance model
 Ftheory
 Fuzzballs
 Graviton
 KaluzaKlein theory
 List of string theory physicists
 List of string theory topics
 Loop quantum gravity
 Mtheory
 Quantum gravity
 Relationship between string theory and quantum field theory
 String duality
 String theory landscape
 Supergravity
 Superstring theory
 Supersymmetry
 Theory of everything
 Zeta function regularization
[edit] References
 ^ M. J. Duff, James T. Liu and R. Minasian Eleven Dimensional Origin of String/String Duality: A One Loop Test Center for Theoretical Physics, Department of Physics, Texas A&M University
 ^ Polchinski, Joseph (1998). String Theory, Cambridge University Press.
 ^ ^{a} ^{b} H. Nastase, The RHIC fireball as a dual black hole, BROWNHET1439, arXiv:hepth/0501068, January 2005,
 ^ ^{a} ^{b} H. Nastase, More on the RHIC fireball and dual black holes, BROWNHET1466, arXiv:hepth/0603176, March 2006,
 ^ ^{a} ^{b} H. Liu, K. Rajagopal, U. A. Wiedemann, An AdS/CFT Calculation of Screening in a Hot Wind, MITCTP3757, arXiv:hepph/0607062 July 2006,
 ^ ^{a} ^{b} H. Liu, K. Rajagopal, U. A. Wiedemann, Calculating the Jet Quenching Parameter from AdS/CFT, Phys.Rev.Lett.97:182301,2006 arXiv:hepph/0605178
 ^ To compare, the size of an atom is roughly 10^{10} m and the size of a proton is 10^{15} m. To imagine the Planck length: you can stretch along the diameter of an atom the same number of strings as the number of atoms you can line up to Proxima Centauri (the nearest star to Earth after the Sun). The tension of a string (8.9×10^{42} newtons) is about 10^{41} times the tension of an average piano string (735 newtons).
 ^ S. James Gates, Jr., Ph.D., Superstring Theory: The DNA of Reality "Lecture 23  Can I Have that Extra Dimension in the Window?", 0:04:54, 0:21:00.
 ^ Simeon Hellerman, Ian Swanson: "Dimensionchanging exact solutions of string theory". ePrint: hepth/0612051; Ofer Aharony, Eva Silverstein: "Supercritical stability, transitions and (pseudo)tachyons". Physical Review D 75:046003, 2007. ePrint: hepth/0612031
 ^ 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 which don't appear in nature. This is known as the linear dilaton or noncritical string.
 ^ "Quantum Geometry of Bosonic Strings – Revisited"
 ^ Aharony, O.; S.S. Gubser, J. Maldacena, H. Ooguri, Y. Oz (2000). "Large N Field Theories, String Theory and Gravity" (subscription required). Phys. Rept. 323: 183–386. doi:. http://arxiv.org/abs/hepth/9905111.. For other examples see: arXiv:hepth/9802042
 ^ For example: T. Sakai and S. Sugimoto, Low energy hadron physics in holographic QCD, Prog.Theor.Phys.113:843882,2005, arXiv:hepth/0412141, December 2004
 ^ See for example Recent Results of the MILC research program, taken from the MILC Collaboration homepage
 ^ David Gross, Perspectives, String Theory: Achievements and Perspectives  A conference
 ^ M. R. Douglas,Are There Testable Predictions of String Theory? February 2007 Texas A&M
 ^ ^{a} ^{b} Peter Woit's Not Even Wrong weblog
 ^ ^{a} ^{b} Lee Smolin's The Trouble With Physics webpage
 ^ John Baez and responses on the group weblog The nCategory Cafe
 ^ John Baez weblog
 ^ Unstrung: The New Yorker
 ^ See e.g. E. Kiritsis, String theory in a nutshell. Introduction to Modern String theory, Princeton University Press, Princeton, N.Y. (2007)
 ^ ^{a} ^{b} ^{c} S. Kachru, R. Kallosh, A. Linde and S. P. Trivedi, de Sitter Vacua in String Theory, Phys.Rev.D68:046005,2003, arXiv:hepth/0301240
 ^ P. Woit (Columbia University), String theory: An Evaluation,February 2001, arXiv:physics/0102051
 ^ P. Woit, Is String Theory Testable? INFN Rome March 2007
 ^ Prominent critics include Philip Anderson ("string theory is the first science in hundreds of years to be pursued in preBaconian fashion, without any adequate experimental guidance", New York Times, 4 January 2005), Sheldon Glashow ("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), Lawrence Krauss ("String theory [is] yet to have any real successes in explaining or predicting anything measurable", New York Times, 8 November 2005), Peter Woit (see his blog, article and book "Not Even Wrong", ISBN 0224076051) and Carlo Rovelli (see his Dialog on Quantum Gravity, arXiv:hepth/0310077)
 ^ N. ArkaniHamed, S. Dimopoulos and S. Kachru, Predictive Landscapes and New Physics at a TeV, arXiv:hepth/0501082, SLACPUB10928, HUTP05A0001, SUITP0444, January 2005
 ^ L. Susskind The Anthropic Landscape of String Theory, arXiv:hepth/0302219, February 2003
 ^ S. James Gates, Jr., Ph.D., Superstring Theory: The DNA of Reality "Lecture 21  Can 4D Forces (without Gravity) Love Strings?", 0:26:060:26:21, cf. 0:24:050:2624.
 ^ Although two decades ago, it was the other way around.
 ^ Idem, "Lecture 19  DoSeeDo and Swing your Superpartner Part II" 0:16:050:24:29.
 ^ Idem, Lecture 21, 0:20:100:21:20.
[edit] Further reading
[edit] Popular books and articles
 Davies, Paul; Julian R. Brown (Eds.) (July 31 1992). Superstrings: A Theory of Everything? (Reprint ed.). Cambridge: Cambridge University Press. pp. 244. ISBN 052143775X.
 Gefter, Amanda (December 2005). "Is string theory in trouble?". New Scientist. http://www.newscientist.com/article/mg18825305.800isstringtheoryintrouble.html?full=true. Retrieved on December 19 2005. – An interview with Leonard Susskind, the theoretical physicist who discovered that string theory is based on onedimensional objects and now is promoting the idea of multiple universes.
 Green, Michael (September 1986). "Superstrings". Scientific American. http://www.damtp.cam.ac.uk/user/mbg15/superstrings/superstrings.html. Retrieved on December 19 2005.
 Greene, Brian (October 20 2003). The Elegant Universe: Superstrings, Hidden Dimensions, and the Quest for the Ultimate Theory (Reissue ed.). New York: W.W. Norton & Company. pp. 464. ISBN 0393058581.
 Greene, Brian (2004). The Fabric of the Cosmos: Space, Time, and the Texture of Reality. New York: Alfred A. Knopf. pp. 569. ISBN 0375412883.
 Gribbin, John (1998). The Search for Superstrings, Symmetry, and the Theory of Everything. London: Little Brown and Company. pp. 224. ISBN 0316329754.
 Halpern, Paul (2004). The Great Beyond: Higher Dimensions, Parallel Universes, and the Extraordinary Search for a Theory of Everything. Hoboken, New Jersey: John Wiley & Sons, Inc.. pp. 326. ISBN 047146595X.
 Hooper, Dan (2006). Dark Cosmos: In Search of Our Universe's Missing Mass and Energy. New York: HarperCollins. pp. 240. ISBN 9780061130328.
 Kaku, Michio (April 1994). Hyperspace: A Scientific Odyssey Through Parallel Universes, Time Warps, and the Tenth Dimension. Oxford: Oxford University Press. pp. 384. ISBN 0195085140.
 Klebanov, Igor and Maldacena, Juan (January 2009). Solving Quantum Field Theories via Curved Spacetimes. Physics Today.
 Musser, George (2008). The Complete Idiot's Guide to String Theory. Indianapolis: Alpha. pp. 368. ISBN 9781592577026.
 Penrose, Roger (February 22 2005). The Road to Reality: A Complete Guide to the Laws of the Universe. Knopf. pp. 1136. ISBN 0679454438. String theory is not the author's preferred approach to unifying physics.
 Randall, Lisa (September 1 2005). Warped Passages: Unraveling the Mysteries of the Universe's Hidden Dimensions. New York: Ecco Press. pp. 512. ISBN 0060531088.
 Susskind, Leonard (December 2006). The Cosmic Landscape: String Theory and the Illusion of Intelligent Design. New York: Hachette Book Group/Back Bay Books. pp. 403. ISBN 0316013331.
 Taubes, Gary (November 1986). "Everything's Now Tied to Strings" Discover Magazine vol 7, #11. (Popular article, probably the first ever written, on the first superstring revolution.)
 Vilenkin, Alex (2006). Many Worlds in One: The Search for Other Universes. New York: Hill and Wang. pp. 235. ISBN 0809095238.
 Witten, Edward (June 2002). "The Universe on a String" (PDF). Astronomy Magazine. http://www.sns.ias.edu/~witten/papers/string.pdf. Retrieved on December 19 2005. – An easy nontechnical article on the very basics of the theory.
Two nontechnical books that are critical of string theory:
 Smolin, Lee (2006). The Trouble with Physics: The Rise of String Theory, the Fall of a Science, and What Comes Next. New York: Houghton Mifflin Co.. pp. 392. ISBN 0618551050.
 Woit, Peter (2006). Not Even Wrong  The Failure of String Theory And the Search for Unity in Physical Law. London: Jonathan Cape &: New York: Basic Books. pp. 290. ISBN 0224076051 & ISBN 9780465092758.
[edit] Textbooks
 Becker, Katrin, Becker, Melanie, and John H. Schwarz (2007) String Theory and MTheory: A Modern Introduction . Cambridge University Press. ISBN 0521860695
 Binétruy, Pierre (2007) Supersymmetry: Theory, Experiment, and Cosmology. Oxford University Press. ISBN 9780198509547.
 Dine, Michael (2007) Supersymmetry and String Theory: Beyond the Standard Model. Cambridge University Press. ISBN 0521858410.
 Paul H. Frampton (1974). Dual Resonance Models. Frontiers in Physics. ISBN 0805325816.
 Gasperini, Maurizio (2007) Elements of String Cosmology. Cambridge University Press. ISBN 9780521868754.
 Michael Green, John H. Schwarz and Edward Witten (1987) Superstring theory. Cambridge University Press. The original textbook.
 Vol. 1: Introduction. ISBN 0521357527.
 Vol. 2: Loop amplitudes, anomalies and phenomenology. ISBN 0521357535.
 Kiritsis, Elias (2007) String Theory in a Nutshell. Princeton University Press. ISBN 9780691122304.
 Johnson, Clifford (2003). Dbranes. Cambridge: Cambridge University Press. ISBN 0521809126.
 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.
 Leonard Susskind, (2006) The Cosmic Landscape: String Theory And The Illusion Of Intelligent Design. Little, Brown & Company ISBN 0316155799
 Szabo, Richard J. (Reprinted 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. Contact author for errata.
[edit] External links
 Superstring Theory Perimeter Institute for Theoretical Physics
 Schwarz, Patricia (1998). "The Official String Theory Web Site". http://superstringtheory.com/. Retrieved on December 16 2005.
 WGBH Educational Foundation (2003). "The Elegant Universe". PBS Online, NOVA. http://www.pbs.org/wgbh/nova/elegant/. Retrieved on December 16 2005. – A ThreeHour Miniseries with Brian Greene by NOVA (original PBS Broadcast Dates: October 28, 810 p.m. and November 4, 89 p.m., 2003). Various images, texts, videos and animations explaining string theory.
 Troost, Jan (2002). "Beyond String Theory". Vrije Universiteit Brussel, Theoretical Physics (TENA). http://tena4.vub.ac.be/beyondstringtheory/. Retrieved on December 16 2005. – An ongoing project by a string physicist, working for the French CNRS.
 Dialogue on the Foundations of String Theory at MathPages
 Pierre, John M. (1999). "Superstrings! String Theory Home Page". http://www.sukidog.com/jpierre/strings/. Retrieved on December 16 2005. – Online tutorial.
 Motl, Luboš; Screiber, Urs. "SCI.physics. STRINGS newsgroup". Harvard High Energy Theory Group. http://schwinger.harvard.edu/~sps/. Retrieved on December 16 2005. – A moderated newsgroup for discussion of string theory (a theory of quantum gravity and unification of forces) and related fields of highenergy physics.
 Schwarz, John H. (2000). "Introduction to Superstring Theory". arXiv.org ePrint archive. http://arxiv.org/abs/hepex/0008017. Retrieved on December 22 2005. – Four lectures, presented at the NATO Advanced Study Institute on Techniques and Concepts of High Energy Physics, St. Croix, Virgin Islands, in June 2000, and addressed to an audience of graduate students in experimental high energy physics, survey basic concepts in string theory.
 Witten, Edward (1998). "Duality, Spacetime and Quantum Mechanics". Kavli Institute for Theoretical Physics. http://online.itp.ucsb.edu/online/plecture/witten/. Retrieved on December 16 2005. – Slides and audio from an Ed Witten lecture where he introduces string theory and discusses its challenges.
 Kibble, Tom (2004). "Cosmic strings reborn?". arXiv.org ePrint archive. http://arxiv.org/abs/astroph/0410073/. Retrieved on December 16 2005. – Invited Lecture at COSLAB 2004, held at Ambleside, Cumbria, United Kingdom, from 10 to 17 September 2004.
 Marolf, Don (2004). "Resource Letter NSST1: The Nature and Status of String Theory". arXiv.org ePrint archive. http://arxiv.org/abs/hepth/0311044/. Retrieved on December 16 2005. – A guide to the string theory literature.
 Ajay, Shakeeb, Wieland et al. (2004). "The nth dimension". http://thenthdimension.com/. Retrieved on December 16 2005. – A comprehensive compilation of materials concerning string theory. Created by an international team of students.
 Woit, Peter (2002). "Is string theory even wrong?". American Scientist. http://www.americanscientist.org/template/AssetDetail/assetid/18638/. Retrieved on December 16 2005. – A criticism of string theory.
 Woit, Peter (2004). "Not Even Wrong". Columbia University Mathematics Department. http://www.math.columbia.edu/~woit/blog/. Retrieved on December 16 2005. – A blog critical of string theory.
 Veneziano, Gabriele (May 2004), "The Myth of the Beginning of Time", Scientific American, http://www.sciam.com/article.cfm?chanID=sa006&articleID=00042F0D1A0E108594F483414B7F0000
 McKie, Robin (20061009), "Setback as string theory of the universe is debunked" (^{[dead link]} – ^{Scholar search}), The Hindu, http://www.hindu.com/thehindu/holnus/008200610091240.htm
 Harris, Richard (20061107). "Short of 'All,' String Theorists Accused of Nothing". National Public Radio. http://www.npr.org/templates/story/story.php?storyId=6377252. Retrieved on 20070305.
 A website dedicated to creative writing inspired by string theory.
 George Gardner (20070124). "Theory of everything put to the test". tech.blorge.com. (Web link). Retrieved on 20070303.
 Minkel, J. R. (20060302), "A Prediction from String Theory, with Strings Attached", Scientific American, http://www.sciam.com/article.cfm?chanId=sa003&articleId=1475A684E7F299DF355B95296BE6031C
 Chalmers, Matthew (20070903). "Stringscape". Physics World. http://physicsworld.com/cws/article/indepth/30940. Retrieved on September 6 2007. — An uptodate and thorough review of string theory in a popular way.
 Smolin, Lee. The Trouble With Physics: The Rise of String Theory, the Fall of a Science, and What Comes Next (2006), Houghton Mifflin. ISBN 9780618551057.
 Woit, Peter. Not Even Wrong: The Failure of String Theory & the Continuing Challenge to Unify the Laws of Physics, 2006. ISBN 0224076051 (Jonathan Cape), ISBN 0465092756 (Basic Books)