# Talk:Mirror symmetry (string theory)

## history of a subject

People who have no clue about the history of a subject should refrain from writing reviews like this one.—Preceding unsigned comment added by 137.138.15.138 (talkcontribs) 13:11, June 29, 2005

## proposed renaming

When I typed in "mirror symmetry", this article popped up instead of Reflection symmetry. I propose renaming this article to something like Mirror symmetry (string theory) or Mirror symmetry (manifolds), so that Mirror symmetry can be a redirect to the more elementary topic in Reflection symmetry. A dab link could be added at the top of that article. Alternatively, Mirror symmetry could be made into a dab page. --Jtir (talk) 12:01, 15 August 2008 (UTC)

There were three articles related to mirror symmetry, so I made Mirror symmetry a dab page.--Jtir (talk) 18:45, 17 August 2008 (UTC)

I have translated into Japanese about 1 year ago. This new article is rewritten from a very "mathematical" view. So in Japanese version the former version is remained as Appendix with sources that are commented out. I will propose that
FIRST, revive the version of july 2013 version as Appendix of this article,
--Enyokoyama (talk) 02:43, 7 September 2013 (UTC)
The current version of the article does emphasize the mathematical applications of mirror symmetry, but I'm still in the process of revising, and eventually I intend to add more about mirror symmetry from a physical point of view. The version from July 2013 was mostly not about mirror symmetry per se but another duality between three-dimensional gauge theories. This information is still available in the article 3D mirror symmetry. Polytope24 (talk) 13:44, 7 September 2013 (UTC)
I hope your description from a physical point of view. However, even if the old description needs several improvements the following items in the old one could not be deleted.

· Batyrev-Borisov construction.

· electromagnetic duality and t'Hooft-Polyakov monopole.

· mirror symmetry in the sigma model on two-dimensional gauge theory.

· mirror symmetry in three-dimensional gauge theory (not be other argicle but in this article.)

They are much important as examples or as applications to string theory. Then I will be revive on this note but not as "Appendix". Please refer.　--Enyokoyama (talk) 14:35, 8 September 2013 (UTC)
I'm afraid I don't know what you're trying to say about an appendix. I'm going to keep adding to this article, and I will talk about the most important physical applications. But the most important thing for right now is to cover the BASIC topics. The previous article had essentially zero discussion of enumerative geometry, which is by far the most famous application of mirror symmetry. The old article was neither well sourced nor accessibly written, and other users have complained about this over at the 3D mirror symmetry article.
Before adding anything about advanced applications to physics, I'm going to add a section on the SYZ conjecture and improve the citations. Mirror symmetry is an enormous topic, and Wikipedia policy requires that the article be written for the widest possible audience without giving undue weight to any particular topic. Polytope24 (talk) 16:09, 8 September 2013 (UTC)
By the way, you are welcome to create subpages on more technical topics and link to them from here. Perhaps that is what you meant by an "appendix". Polytope24 (talk) 16:13, 8 September 2013 (UTC)
Thanks! Mr. Polytope24. Firstly, I will only revive the previous version at July 2013 on this note, though they needs some improvements.--Enyokoyama (talk) 22:20, 8 September 2013 (UTC)

Now, I will post the version of "mirror symmetry (string)" at 1st Aug 2013 as a new section, which is the previous version of this from the rather physical view point. I think that this article needs some improvement.--Enyokoyama (talk) 15:12, 10 September 2013 (UTC)

Dear Mr Polytope24!　I agree with you completely. The 1st Aug 2013 version has some problematic parts as an article and needs significant improvements. Part of the "Mirror symmetry in 3-dimensional gauge theories" becomes a separate article and I will modify to refer to the separate article. I will never disturb this article.--Enyokoyama (talk) 13:08, 12 September 2013 (UTC)

## the 1st Aug 2013 version of this article "mirror symmetry (string theory)"

In physics and mathematics, mirror symmetry is a relation that can exist between two Calabi–Yau manifolds. It happens, usually for two such six-dimensional manifolds, that the shapes may look very different geometrically, but nevertheless they are equivalent if they are employed as hidden dimensions of string theory. The classical formulation of mirror symmetry relates two Calabi–Yau threefolds M and W whose Hodge numbers h1,1 and h1,2 are swapped; string theory compactified on these two manifolds lead to identical effective field theories.

## History

The discovery of mirror symmetry is connected with names such as Lance Dixon, Wolfgang Lerche, Cumrun Vafa, Nicholas Warner, Brian Greene, Ronen Plesser, Philip Candelas, Monika Lynker, Rolf Schimmrigk and others. Andrew Strominger, Shing-Tung Yau, and Eric Zaslow have showed that mirror symmetry is a special example of T-duality: the Calabi–Yau manifold may be written as a fiber bundle whose fiber is a three-dimensional torus. The simultaneous action of T-duality on all three dimensions of this torus is equivalent to mirror symmetry.

Mathematicians became interested in mirror symmetry in 1990, after Candelas-de la Ossa-Green-Parkes gave predictions for numbers of rational curves in a quintic threefold via data coming from variation of Hodge structure on the mirror family. These predictions were mathematically proven a few years later by Alexander Givental and Lian-Liu-Yau.

## Applications

Mirror symmetry allowed the physicists to calculate many quantities that seemed virtually incalculable before, by invoking the "mirror" description of a given physical situation, which can be often much easier. Mirror symmetry has also become a tool in mathematics, and although mathematicians have proved theorems based on the physicists' intuition, a full mathematical understanding of the phenomenon of mirror symmetry is still being developed.

Most of the physical examples can be conceptualized by the Batyrev–Borisov mirror construction, which uses the duality of reflexive polytopes and nef partitions. In their construction the mirror partners appear as anticanonically embedded hypersurfaces or certain complete intersections in Fano toric varieties. The Gross–Siebert mirror construction generalizes this to non-embedded cases by looking at degenerating families of Calabi–Yau manifolds. This point of view also includes T-duality. Another mathematical framework is provided by the homological mirror symmetry conjecture.

## Generalizations

There are two different, but closely related, string theory statements of mirror symmetry.[1]

1. Type IIA string theory on a Calabi–Yau M is mirror dual to Type IIB on W.
2. Type IIB string theory on a Calabi–Yau M is mirror dual to Type IIA on W.

This follows from the fact that Calabi–Yau hodge numbers satisfy h1,1 ${\displaystyle \geq }$ 1 but h2,1\${\displaystyle \geq }$ 0. If the Hodge numbers of M are such that h2,1=0 then by definition its mirror dual W is not Calabi–Yau. As a result mirror symmetry allows for the definition of an extended space of compact spaces, which are defined by the W of the above two mirror symmetries.

Mirror symmetry has also been generalized to a duality between supersymmetric gauge theories in various numbers of dimensions. In this generalized context the original mirror symmetry, which relates pairs of toric Calabi–Yau manifolds, relates the moduli spaces of 2-dimensional abelian supersymmetric gauge theories when the sums of the electric charges of the matter are equal to zero.

In all manifestations of mirror symmetry found so far a central role is played by the fact that in a d-dimensional quantum field theory a differential p-form potential admits a dual formulation as a (d-p-2)-form potential. In 4-dimensions this relates the electric and magnetic vector potentials and is called electric–magnetic duality. In 3-dimensions this duality relates a vector and a scalar, which in an abelian gauge theory correspond to a photon and a squark. In 2-dimensions it relates two scalars, but while one carries an electric charge, the dual scalar is an uncharged Fayet-Iliopoulos term. In the process of this duality topological solitons called Abrikosov-Nielsen-Oleson vortices are intercharged with elementary quark fields in the 3-dimensional case and play the role in instantons in the 2-dimensional case.

The derivations of 2-dimensional mirror symmetry and 3-dimensional mirror symmetry are both inspired by Alexander Polyakov's instanton calculation in non-supersymmetric quantum electrodynamics with a scalar Higgs field. In a 1977 article[2] he demonstrated that instanton effects give the photon a mass, where the instanton is a 't Hooft-Polyakov monopole embedded in an ultraviolet nonabelian gauge group.

## Mirror symmetry in 2-dimensional gauged sigma models

Mirror symmetries in 2-dimensional sigma models are usually considered in cases with N=(2,2) supersymmetry, which means that the fermionic supersymmetry generators are the four real components of a single Dirac spinor. This is the case which is relevant, for example, to topological string theories and type II superstring theory. Generalizations to N=(2,0) supersymmetry have also appeared.[3]

The matter content of N=(2,2) gauged linear sigma models consists of three kinds of supermultiplet. The gauge bosons occur in vector multiplets, the charged matter occurs in chiral multiplets and the Fayet-Ilipolous (FI) terms of the various abelian gauge symmetries occur in twisted chiral multiplets. Mirror symmetry exchanges chiral and twisted chiral multiplets.

Mirror symmetry, in a class of models of toric varieties with zero first Chern class Calabi–Yau manifolds and positive first Chern class (Fano varieties) was proven by Kentaro Hori and Cumrun Vafa.[4] Their approach is as follows. A sigma model whose target space is a toric variety may be described by an abelian gauge theory with charged chiral multiplets. Mirror symmetry then replaces these charged chiral multiplets with uncharged twisted chiral multiplets whose vacuum expectation values are FI terms. Instantons in the dual theory are now vortices whose action is given by the exponential of the FI term. These vortices each have precisely 2 fermion zeromodes, and so the sole correction to the superpotential is given by a single vortex. The nonperturbative corrections to the dual superpotential may then be found by simply summing the exponentials of the FI terms. Therefore mirror symmetry allows one to find the full nonperturbative solutions to the theory.

In addition to finding many new dualities, this allowed them to demonstrate many dualities that had been conjectured in the literature. For example, beginning with a sigma model whose target space is the 2-sphere they found an exactly solvable Sine-Gordon model. More generally, when the original sigma model's target space is the n-complex dimensional projective space they found that the dual theory is the exactly solvable affine Toda model.

## Mirror symmetry in 3-dimensional gauge theories

### Notes

1. In Section 9.9 of 'String Theory and M theory' by Becker, Becker and Schwarz
2. Quark Confinement and Topology of Gauge Groups
3. For example in (0,2) duality.
4. In the paper Mirror Symmetry.

### References

• Strominger, Andrew; Yau, Shing-Tung; Zaslow, Eric, "Mirror Symmetry is T-duality" hep-th/9606040
• Cox, David A.; Katz, Sheldon, Mirror symmetry and algebraic geometry. Mathematical Surveys and Monographs, 68. American Mathematical Society, Providence, RI, 1999. xxii+469 pp. ISBN 0-8218-1059-6
• Hori, Kentaro; Katz, Sheldon; Klemm, Albrecht; Pandharipande, Rahul; Thomas, Richard; Vafa, Cumrun; Vakil, Ravi; Zaslow, Eric Mirror symmetry. Clay Mathematics Monographs, 1. American Mathematical Society, Providence, RI; Clay Mathematics Institute, Cambridge, MA, 2003. xx+929 pp. ISBN 0-8218-2955-6
• Victor Batyrev; Dual Polyhedra and for Calabi-Yau Hypersurfaces in Toric Varieties J. Algebraic Geom. 3 (1994), no. 3, 493—535
• Mark Gross; Toric Degenerations and Batyrev-Borisov Duality: [1]