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Related papers: M(atrix)-Theory in Various Dimensions

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We consider M(atrix) theory compactifications to seven dimensions with eight unbroken supersymmetries. We conjecture that both M(atrix) theory on K3 and Heterotic M(atrix) theory on T^3 are described by the same 5+1 dimensional theory with…

High Energy Physics - Theory · Physics 2016-08-25 Suresh Govindarajan

In the M(atrix) theory by making the expansions of the matrices around the membrane and four-brane solutions we derive the three- and five-dimensional gauge theories on the dual tori. The explicit forms of solutions yield the dual…

High Energy Physics - Theory · Physics 2010-11-19 Shijong Ryang

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

We calculate the potential between various configurations of membranes and gravitons in M(atrix) theory. The computed potentials agree with the short distance potentials between corresponding 2-branes and 0-brane configurations in Type IIA…

High Energy Physics - Theory · Physics 2009-10-30 Gilad Lifschytz , Samir D. Mathur

We suggest and motivate a precise equivalence between uncompactified eleven dimensional M-theory and the N = infinity limit of the supersymmetric matrix quantum mechanics describing D0-branes. The evidence for the conjecture consists of…

High Energy Physics - Theory · Physics 2009-07-09 T. Banks , W. Fischler , S. H. Shenker , L. Susskind

We use the T-duality transformation which relates M-theory on T^3 to M-theory on a second T^3 with inverse volume to test the Banks-Fischler-Shenker-Susskind suggestion for the matrix model description of M-theory. We find evidence that…

High Energy Physics - Theory · Physics 2008-11-26 Ori J. Ganor , Sanjaye Ramgoolam , Washington Taylor

We study compactifications of string theory and M-theory to six dimensions with background fluxes. The nonzero fluxes lead to additional mass parameters. We derive the S- and T-duality rules for the corresponding (massive) supergravity…

High Energy Physics - Theory · Physics 2008-12-18 K. Behrndt , E. Bergshoeff , D. Roest , P. Sundell

The issue of justifying the matrix-theory proposal is revisited. We first discuss how the matrix-string theory is derived directly starting from the eleven dimensional supermembrane wrapped around a circle of radius $R=g_s\ell_s$, without…

High Energy Physics - Theory · Physics 2007-05-23 Tamiaki Yoneya

We study M(atrix) theory description of M theory compactified on T5/Z2 orbifold. In the large volume limit we show that M theory dynamics is described by N=8 supersymmetric USp(2N) M(atrix) quantum mechanics. Via zero-brane parton…

High Energy Physics - Theory · Physics 2009-10-30 N. Kim , Soo-Jong Rey

We demonstrate the emergence of the U-duality group in compactification of Matrix theory on a 4-torus. The discussion involves non-trivial effects in strongly coupled 4+1 dimensional gauge theory, and highlights some interesting phenomena…

High Energy Physics - Theory · Physics 2009-10-30 Moshe Rozali

M(atrix) theory description is investigated for M-theory compactified on non-orientable manifolds. Relevant M(atrix) theory is obtained by Fourier transformation in a way consistent with T-duality. For nine-dimensional compactification on…

High Energy Physics - Theory · Physics 2007-05-23 N. Kim , Soo-Jong Rey

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

Membrane scattering in m(atrix) theory is related to dynamics in three-dimensional $SU(2)$ gauge theory, with transfer of $p^{11}$ being an instanton process. We calculate the instanton amplitude and find precise agreement with the…

High Energy Physics - Theory · Physics 2009-10-09 Joseph Polchinski , Philippe Pouliot

The nature of M-theory on K3 X I, where I is a line interval, is considered, with a view towards formulating a `matrix theory' representation of that situation. Various limits of this compactification of M-theory yield a number of well…

High Energy Physics - Theory · Physics 2009-10-30 Clifford V. Johnson

We derive the noncommutative torus compactification of M(atrix) theory directly from the string theory by imposing mixed boundary conditions on the membranes. The relation of various dualities in string theory and M(atrix) theory…

High Energy Physics - Theory · Physics 2007-05-23 F. Ardalan , H. Arfaei , M. M. Sheikh-Jabbari

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

We consider membranes of spherical topology in uncompactified Matrix theory. In general for large membranes Matrix theory reproduces the classical membrane dynamics up to 1/N corrections; for certain simple membrane configurations, the…

High Energy Physics - Theory · Physics 2008-11-26 Daniel Kabat , Washington Taylor

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

Compactifications of M-theory to two dimensional space-time on ${(K3\times \T^5)}/ \Z_2$ and ${(K3\times K3\times \S^1)}/ \Z_2$ orientifolds are presented. These orientifolds provide examples of anomaly free chiral supergravity models in…

High Energy Physics - Theory · Physics 2009-10-30 Alok Kumar , Koushik Ray

We present M-theory compactifications on $K_3 \times K_3$ with membranes near the $A_n$ or $D_n$ singularities of the $K_3$ spaces. By realizing each of these compactifications in two different ways as type I' models with 2- and 6-branes,…

High Energy Physics - Theory · Physics 2009-10-30 M. Porrati , A. Zaffaroni
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