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Related papers: Non-Orientable M(atrix) Theory

200 papers

We construct the Matrix theory descriptions of M-theory on the Mobius strip and the Klein bottle. In a limit, these provide the matrix string theories for the CHL string and an orbifold of type IIA string theory.

High Energy Physics - Theory · Physics 2009-10-30 Gysbert Zwart

We study orbifold compactifications of F-theory which lead to $N=1$ supersymmetry in 6 and 4 spacetime dimensions. These are dual to specific orientifolds of M-theory, and in many cases to orientifolds of type IIB string theory. The…

High Energy Physics - Theory · Physics 2009-10-30 Rajesh Gopakumar , Sunil Mukhi

We construct several examples of compactification of Type IIB theory on orientifolds and discuss their duals. In six dimensions we obtain models with $N=1$ supersymmetry, multiple tensor multiplets, and different gauge groups. In nine…

High Energy Physics - Theory · Physics 2009-10-30 Atish Dabholkar , Jaemo Park

We study a class of compactifications of M-theory to three dimensions that preserve N=2 supersymmetry and which have the defining feature that a probe space-time filling M2 brane feels a non-trivial potential on the internal manifold. Using…

High Energy Physics - Theory · Physics 2015-06-18 Cezar Condeescu , Andrei Micu , Eran Palti

We study Z2-orbifolds of 11-dimensional M-theory on tori of various dimensions. The most interesting model (besides the known S1/Z2 case) corresponds to T5/Z2, for which we argue that the resulting six-dimensional theory is equivalent to…

High Energy Physics - Theory · Physics 2009-10-28 Keshav Dasgupta , Sunil Mukhi

We consider compactifications of the matrix model of M-theory on $S^1/Z_2\times T^d$ for $d>0$, and interpret them as orbifolds of the supersymmetric U(N) Yang-Mills theory on $R\times T^{d+1}$. The orbifold group acts both on the gauge…

High Energy Physics - Theory · Physics 2016-09-06 Petr Horava

We consider several orbifold compactifications of M-theory and their corresponding type II duals in two space-time dimensions. In particular, we show that while the orbifold compactification of M-theory on $T^9/J_9$ is dual to the orbifold…

High Energy Physics - Theory · Physics 2010-11-19 Shibaji Roy

In this paper we study duality properties of the M(atrix) theory compactified on a circle. We establish the equivalence of this theory to the strong coupling limit of type IIB string theory compactified on a circle. In the M(atrix) theory…

High Energy Physics - Theory · Physics 2009-10-30 Pei-Ming Ho , Yong-Shi Wu

After a short introduction to Matrix theory, we explain how can one generalize matrix models to describe toroidal compactifications of M-theory and the heterotic vacua with 16 supercharges. This allows us, for the first time in history, to…

High Energy Physics - Theory · Physics 2007-05-23 Lubos Motl

This diploma thesis has three major objectives. Firstly, we give an elementary introduction to M-theory compactifications, which are obtained from an analysis of its low-energy effective theory, eleven-dimensional supergravity. In…

High Energy Physics - Theory · Physics 2007-05-23 Steffen Metzger

We study a decoupling limit of M-theory where the three-form gauge potential becomes critical. This limit leads to nonrelativistic M-theory coupled to a non-Lorentzian spacetime geometry. Nonrelativistic M-theory is U-dual to M-theory in…

High Energy Physics - Theory · Physics 2023-11-27 Stephen Ebert , Ziqi Yan

By identifying the moduli space of coupling constants in the SYM description of toroidal compactifications of M(atrix)-Theory, we construct the M(atrix) description of the moduli spaces of Type IIA string theory compactified on T^n.…

High Energy Physics - Theory · Physics 2010-11-19 David Berenstein , Richard Corrado , Jacques Distler

We discuss M(atrix) theory compactification on T^6. This theory is described by the large N limit of the world volume theory, of N Kaluza-Klein monopoles in eleven dimensions. We discuss the BPS states, and their arrangement in E_6…

High Energy Physics - Theory · Physics 2014-11-18 Amihay Hanany , Gilad Lifschytz

We study compactifications of Matrix theory on twisted tori and non-commutative versions of them. As a first step, we review the construction of multidimensional twisted tori realized as nilmanifolds based on certain nilpotent Lie algebras.…

High Energy Physics - Theory · Physics 2013-05-30 Athanasios Chatzistavrakidis , Larisa Jonke

We study explicit solutions for orientifolds of Matrix theory compactified on noncommutative torus. As quotients of torus, cylinder, Klein bottle and M\"obius strip are applicable as orientifolds. We calculate the solutions using Connes,…

High Energy Physics - Theory · Physics 2010-11-19 Nakwoo Kim

We study a new class of matrix models, the simplest of which is based on an Sp(2) symmetry and has a compactification which is equivalent to Chern-Simons theory on the three-torus. By replacing Sp(2) with the super-algebra Osp(1|32), which…

High Energy Physics - Theory · Physics 2014-11-18 Lee Smolin

Motivated by the description of $\mathcal{N}=1$ M-theory compactifications to four-dimensions given by Exceptional Generalized Geometry, we propose a way to geometrize the M-theory fluxes by appropriately relating the compactification space…

High Energy Physics - Theory · Physics 2015-04-07 Mariana Graña , C. S. Shahbazi

This work is devoted to a study of some of the non-perturbative aspects of superstring theory that have come within reach thanks to dualities. The first chapter gives a non-technical zero-equation introduction to these developments intended…

High Energy Physics - Theory · Physics 2007-05-23 B. Pioline

T duality expresses the equivalence of a superstring theory compactified on a manifold K to another (possibly the same) superstring theory compactified on a dual manifold K'. The volumes of K and K' are inversely proportional. In this talk…

High Energy Physics - Theory · Physics 2007-05-23 John H. Schwarz

We compute the mass and multiplet spectrum of M theory compactified on the product of AdS(4) spacetime by the Stiefel manifold V(5,2)=SO(5)/SO(3), and we use this information to deduce via the AdS/CFT map the primary operator content of the…

High Energy Physics - Theory · Physics 2009-10-31 A. Ceresole , G. Dall'Agata , R. D'Auria , S. Ferrara