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      Supersymmetric Yang-Mills Systems And Integrable Systems

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          Abstract

          The Coulomb branch of \(N=2\) supersymmetric gauge theories in four dimensions is described in general by an integrable Hamiltonian system in the holomorphic sense. A natural construction of such systems comes from two-dimensional gauge theory and spectral curves. Starting from this point of view, we propose an integrable system relevant to the \(N=2\) \(SU(n)\) gauge theory with a hypermultiplet in the adjoint representation, and offer much evidence that it is correct. The model has an \(SL(2,{\bf Z})\) \(S\)-duality group (with the central element \(-1\) of \(SL(2,{\bf Z})\) acting as charge conjugation); \(SL(2,{\bf Z})\) permutes the Higgs, confining, and oblique confining phases in the expected fashion. We also study more exotic phases.

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          The Vacuum Structure and Spectrum of N=2 Supersymmetric SU(N) Gauge Theory

          We present an exact description of the metric on the moduli space of vacua and the spectrum of massive states for four dimensional N=2 supersymmetric SU(n) gauge theories. The moduli space of quantum vacua is identified with the moduli space of a special set of genus n-1 hyperelliptic Riemann surfaces.
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            Author and article information

            Journal
            16 October 1995
            1995-10-23
            Article
            10.1016/0550-3213(95)00609-5
            hep-th/9510101
            caec3487-58d7-444e-858c-d9a678b081a4
            History
            Custom metadata
            Nucl.Phys.B460:299-334,1996
            50 pages, harvmac. added references
            hep-th alg-geom math.AG

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