Abstract
We study supersymmetric Chern-Simons with fundamental and antifundamental chiral multiplets of mass in the complete parameter space spanned by , where denotes the coupling constant. In particular, we analyze the matrix model description of its partition function, both at finite using the method of orthogonal polynomials together with Mordell integrals and, at large with fixed , using the theory of Toeplitz determinants. We show for the massless case that there is an explicit realization of the Giveon-Kutasov duality. For finite , with , three regimes that exactly correspond to the known three large phases of theory are identified and characterized.
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