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The Matrix model and the non-commutative geometry of the supermembrane

This is a short note on the relation of the Matrix model with the non-commutative geometry of the 11-dimensional supermembrane. We put forward the idea that M-theory is described by the t' Hooft topological expansion of the Matrix model in the large N-limit where all topologies of membranes app...

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Autores principales: Floratos, E.G., Leontaris, G.K.
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(99)01036-9
http://cds.cern.ch/record/396748
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author Floratos, E.G.
Leontaris, G.K.
author_facet Floratos, E.G.
Leontaris, G.K.
author_sort Floratos, E.G.
collection CERN
description This is a short note on the relation of the Matrix model with the non-commutative geometry of the 11-dimensional supermembrane. We put forward the idea that M-theory is described by the t' Hooft topological expansion of the Matrix model in the large N-limit where all topologies of membranes appear. This expansion can faithfully be represented by the Moyal Yang-Mills theory of membranes. We discuss this conjecture in the case of finite N, where the non-commutative geometry of the membrane is given be the finite quantum mechanics. The use of the finite dimensional representations of the Heisenberg group reveals the cellular structure of a toroidal supemembrane on which the Matrix model appears as a non-commutatutive Yang-Mills theory. The Moyal star product on the space of functions in the case of rational values of Planck constant \hbar represents exactly this cellular structure. We also discuss the integrability of the instanton sector as well as the topological charge and the corresponding Bogomol'nyi bound.
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spelling cern-3967482023-03-14T19:54:39Zdoi:10.1016/S0370-2693(99)01036-9http://cds.cern.ch/record/396748engFloratos, E.G.Leontaris, G.K.The Matrix model and the non-commutative geometry of the supermembraneParticle Physics - TheoryThis is a short note on the relation of the Matrix model with the non-commutative geometry of the 11-dimensional supermembrane. We put forward the idea that M-theory is described by the t' Hooft topological expansion of the Matrix model in the large N-limit where all topologies of membranes appear. This expansion can faithfully be represented by the Moyal Yang-Mills theory of membranes. We discuss this conjecture in the case of finite N, where the non-commutative geometry of the membrane is given be the finite quantum mechanics. The use of the finite dimensional representations of the Heisenberg group reveals the cellular structure of a toroidal supemembrane on which the Matrix model appears as a non-commutatutive Yang-Mills theory. The Moyal star product on the space of functions in the case of rational values of Planck constant \hbar represents exactly this cellular structure. We also discuss the integrability of the instanton sector as well as the topological charge and the corresponding Bogomol'nyi bound.This is a short note on the relation of the Matrix model with the non-commutative geometry of the 11-dimensional supermembrane. We put forward the idea that M-theory is described by the 't Hooft topological expansion of the Matrix model in the large N-limit where all topologies of membranes appear. This expansion can faithfully be represented by the Moyal Yang-Mills theory of membranes. We discuss this conjecture in the case of finite N, where the non-commutative geometry of the membrane is given be the finite quantum mechanics. The use of the finite dimensional representations of the Heisenberg group reveals the cellular structure of a toroidal supermembrane on which the Matrix model appears as a non-commutatutive Yang-Mills theory. The Moyal star product on the space of functions in the case of rational values of the Planck constant \hbar represents exactly this cellular structure. We also discuss the integrability of the instanton sector as well as the topological charge and the corresponding Bogomol'nyi bound.This is a short note on the relation of the Matrix model with the non-commutative geometry of the 11-dimensional supermembrane. We put forward the idea that M-theory is described by the 't Hooft topological expansion of the Matrix model in the large N -limit where all topologies of membranes appear. This expansion can faithfully be represented by the Moyal Yang-Mills theory of membranes. We discuss this conjecture in the case of finite N , where the non-commutative geometry of the membrane is given be the finite quantum mechanics. The use of the finite dimensional representations of the Heisenberg group reveals the cellular structure of a toroidal supermembrane on which the Matrix model appears as a non-commutatutive Yang–Mills theory. The Moyal star product on the space of functions in the case of rational values of the Planck constant ℏ represents exactly this cellular structure. We also discuss the integrability of the instanton sector as well as the topological charge and the corresponding Bogomol'nyi bound.hep-th/9908106CERN-TH-99-251oai:cds.cern.ch:3967481999-08-17
spellingShingle Particle Physics - Theory
Floratos, E.G.
Leontaris, G.K.
The Matrix model and the non-commutative geometry of the supermembrane
title The Matrix model and the non-commutative geometry of the supermembrane
title_full The Matrix model and the non-commutative geometry of the supermembrane
title_fullStr The Matrix model and the non-commutative geometry of the supermembrane
title_full_unstemmed The Matrix model and the non-commutative geometry of the supermembrane
title_short The Matrix model and the non-commutative geometry of the supermembrane
title_sort matrix model and the non-commutative geometry of the supermembrane
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/S0370-2693(99)01036-9
http://cds.cern.ch/record/396748
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