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Related papers: Modified pure spinors and mirror symmetry

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Certain limits of the duality between M-theory on ${T^5/Z_2}$ and IIB on K3 are analyzed in Matrix theory. The correspondence between M-theory five-branes and ALE backgrounds is realized as three dimensional mirror symmetry. Non-critical…

High Energy Physics - Theory · Physics 2010-11-19 Duiliu-Emanuel Diaconescu , Jaume Gomis

By applying mirror symmetry to D-branes in a Calabi-Yau geometry we shed light on a $G_2$ flop in M-theory relevant for large $N$ dualities in ${\cal N}=1$ supersymmetric gauge theories. Furthermore, we derive superpotential for M-theory on…

High Energy Physics - Theory · Physics 2009-11-07 Mina Aganagic , Cumrun Vafa

These notes are devoted to explaining aspects of the mirror manifold problem that can be naturally understood from the point of view of topological field theory. Basically this involves studying the topological field theories made by…

High Energy Physics - Theory · Physics 2007-05-23 Edward Witten

It is shown that in string theory mirror duality is a gauge symmetry (a Weyl transformation) in the moduli space of $N=2$ backgrounds on group manifolds, and we conjecture on the possible generalization to other backgrounds, such as…

High Energy Physics - Theory · Physics 2010-04-07 Amit Giveon , Edward Witten

We describe the construction of configurations of D6-branes wrapped on compact 3-cycles intersecting at points in non-compact Calabi-Yau threefolds. Such constructions provide local models of intersecting brane worlds, and describe sectors…

High Energy Physics - Theory · Physics 2009-11-07 Angel M. Uranga

We give geometric explanations and proofs of various mirror symmetry conjectures for $T^{n}$-invariant Calabi-Yau manifolds when instanton corrections are absent. This uses fiberwise Fourier transformation together with base Legendre…

Differential Geometry · Mathematics 2007-05-23 Naichung Conan Leung

We introduce a notion of twisted pure spinor in order to characterize, in a unified way, all the special Riemannian holonomy groups just as a classical pure spinor characterizes the special K\"ahler holonomy. Motivated by certain curvature…

Differential Geometry · Mathematics 2019-09-24 Rafael Herrera , Noemi Santana

We describe supersymmetric A-branes and B-branes in open N=(2,2) dynamically gauged nonlinear sigma models (GNLSM), placing emphasis on toric manifold target spaces. For a subset of toric manifolds, these equivariant branes have a mirror…

High Energy Physics - Theory · Physics 2018-03-21 Meer Ashwinkumar , Meng-Chwan Tan

Using D2-brane probes, we study various properties of M-theory on singular, non-compact manifolds of G_2 and Spin(7) holonomy. We derive mirror pairs of N=1 supersymmetric three-dimensional gauge theories, and apply this technique to…

High Energy Physics - Theory · Physics 2009-11-07 Sergei Gukov , David Tong

We show that the supersymmetry transformations for type II string theories on six-manifolds can be written as differential conditions on a pair of pure spinors, the exponentiated Kahler form exp(iJ) and the holomorphic form Omega. The…

High Energy Physics - Theory · Physics 2008-11-26 Mariana Grana , Ruben Minasian , Michela Petrini , Alessandro Tomasiello

D-branes can end on orbifold planes if the action of the orbifold group includes (-1)^{F_L}. We consider configurations of D-branes ending on such orbifolds and study the low-energy theory on their worldvolume. We apply our results to gauge…

High Energy Physics - Theory · Physics 2010-02-03 Anton Kapustin

The recent result of Strominger, Yau and Zaslow relating mirror symmetry to the quantum field theory notion of T-duality is reinterpreted as providing a way of geometrically characterizing which Calabi-Yau manifolds have mirror partners.…

alg-geom · Mathematics 2008-02-03 David R. Morrison

We consider the asymmetric orbifold that is obtained by acting with T-duality on a 4-torus, together with a shift along an extra circle. The chiral algebra of the resulting theory has non-trivial outer automorphisms that act as permutations…

High Energy Physics - Theory · Physics 2010-04-05 Matthias R Gaberdiel , Sakura Schafer-Nameki

We discuss pseudoduality transformations in two dimensional conformally invariant classical sigma models, and extend our analysis to a given boundaries of world-sheet, which gives rise to an appropriate framework for the discussion of the…

High Energy Physics - Theory · Physics 2013-06-20 Mustafa Sarisaman

We define spin frames, with the aim of extending spin structures from the category of (pseudo-)Riemannian manifolds to the category of spin manifolds with a fixed signature on them, though with no selected metric structure. Because of this…

Differential Geometry · Mathematics 2019-10-11 R. Noris , L. Fatibene

We perform a Hodge theoretic study of parameter dependent families of D-branes on compact Calabi-Yau manifolds in type II and F-theory compactifcations. Starting from a geometric Gauss-Manin connection for B type branes we study the…

High Energy Physics - Theory · Physics 2010-09-24 Murad Alim , Michael Hecht , Hans Jockers , Peter Mayr , Adrian Mertens , Masoud Soroush

We generalize the free Fermi-gas formulation of certain 3d ${\cal N}=3$ supersymmetric Chern-Simons-matter theories by allowing Fayet-Iliopoulos couplings as well as mass terms for bifundamental matter fields. The resulting partition…

High Energy Physics - Theory · Physics 2015-10-14 Nadav Drukker , Jan Felix

We extend previous results on generalized calibrations to describe supersymmetric branes in supergravity backgrounds with diverse fields turned on, and provide several new classes of examples. As an important application, we show that…

High Energy Physics - Theory · Physics 2009-10-09 Juan F. G. Cascales , Angel M. Uranga

When combined with mirror symmetry, the A-model approach to quantization leads to a fairly simple and tractable problem. The most interesting part of the problem then becomes finding the mirror of the coisotropic brane. We illustrate how it…

High Energy Physics - Theory · Physics 2011-06-07 Sergei Gukov

The two discrete generators of the full Lorentz group $O(1,3)$ in $4D$ spacetime are typically chosen to be parity inversion symmetry $P$ and time reversal symmetry $T$, which are responsible for the four topologically separate components…

General Physics · Physics 2023-07-17 Wanpeng Tan