266 research outputs found

    Confining Phase of N=1 Sp(Nc)Sp(N_c) Gauge Theories via M Theory Fivebrane

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    The moduli space of vacua for the confining phase of N=1 Sp(Nc)Sp(N_c) supersymmetric gauge theories in four dimensions is studied by M theory fivebrane. We construct M theory fivebrane configuration corresponding to the perturbation of superpotential in which the power of adjoint field is related to the number of NS'5 branes in type IIA brane configuration. We interpret the dyon vacuum expectation values in field theory results as the brane geometry and the comparison with meson vevs will turn out that the low energy effective superpotential with enhanced gauge group SU(2) is exact.Comment: 14 pages, late

    Geometry, D-Branes and N=1 Duality in Four Dimensions II

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    We study N=1 dualities in four dimensional supersymmetric gauge theories in terms of wrapping D 6-branes around 3-cycles of Calabi-Yau threefolds in type IIA string theory. We generalize the recent work of geometrical realization for the models which have the superpotential corresponding to an AkA_k type singularity, to various models presented by Brodie and Strassler, consisting of Dk+2D_{k+2} superpotential of the form W=TrXk+1+TrXY2W=Tr X^{k+1} + Tr XY^2. We discuss a large number of representations for the field YY, but with XX always in the adjoint (symmetric) [antisymmetric] representation for SU(SO)[Sp]SU (SO) [Sp] gauge groups.Comment: 15 pages, late

    c=5/2 Free Fermion Model of WB_{2} Algebra

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    We investigate the explicit construction of the WB2WB_{2} algebra, which is closed and associative for all values of the central charge cc, using the Jacobi identity and show the agreement with the results studied previously. Then we illustrate a realization of c=52c=\frac{5}{2} free fermion model, which is m→∞m \rightarrow \infty limit of unitary minimal series, c(WB2)=52(1−12(m+3)(m+4))c ( WB_{2} )=\frac{5}{2} (1-\frac{12}{ (m+3)(m+4) }) based on the cosets (B2^⊕B2^,B2^)( \hat{B_{2}} \oplus \hat{B_{2}}, \hat{B_{2} }) at level (1,m).(1,m). We confirm by explicit computations that the bosonic currents in the WB2 WB_{2} algebra are indeed given by the Casimir operators of B2^\hat{B_{2}} .Comment: 16 page
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