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      Noncommutative Field Theory

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          Abstract

          We review the generalization of field theory to space-time with noncommuting coordinates, starting with the basics and covering most of the active directions of research. Such theories are now known to emerge from limits of M theory and string theory, and to describe quantum Hall states. In the last few years they have been studied intensively, and many qualitatively new phenomena have been discovered, both on the classical and quantum level. To appear in Reviews of Modern Physics.

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          M Theory As A Matrix Model: A Conjecture

          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 several correspondences between the two theories. As a consequence of supersymmetry the simple matrix model is rich enough to describe the properties of the entire Fock space of massless well separated particles of the supergravity theory. In one particular kinematic situation the leading large distance interaction of these particles is exactly described by supergravity . The model appears to be a nonperturbative realization of the holographic principle. The membrane states required by M-theory are contained as excitations of the matrix model. The membrane world volume is a noncommutative geometry embedded in a noncommutative spacetime.
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            Dirichlet-Branes and Ramond-Ramond Charges

            We show that Dirichlet-branes, extended objects defined by mixed Dirichlet-Neumann boundary conditions in string theory, break half of the supersymmetries of the type~II superstring and carry a complete set of electric and magnetic Ramond-Ramond charges. We also find that the product of the electric and magnetic charges is a single Dirac unit, and that the quantum of charge takes the value required by string duality. This is strong evidence that the Dirchlet-branes are intrinsic to type II string theory and are the Ramond-Ramond sources required by string duality. We also note the existence of a previously overlooked 9-form potential in the IIa string, which gives rise to an effective cosmological constant of undetermined magnitude.
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              A planar diagram theory for strong interactions

              G.'t Hooft (1974)
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                Author and article information

                Journal
                06 June 2001
                2001-10-18
                Article
                10.1103/RevModPhys.73.977
                hep-th/0106048
                2ec3485e-c123-4e18-a4f6-9047fb3a5452
                History
                Custom metadata
                ITEP-TH-31/01, IHES/P/01/27, RUNHETC-2001-18
                Rev.Mod.Phys.73:977-1029,2001
                Revtex, 56 pp, 6 figures. Final version
                hep-th

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