118 research outputs found

    Finite Size Effects and Conformal Symmetry of O(N)O(N) Nonlinear σ\sigma Model in Three Dimensions

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    We study the O(N)O(N) nonlinear σ\sigma model on a three-dimensional compact space S1×S2S^1 \times S^2 (of radii LL and RR respectively) by means of large NN expansion, focusing on the finite size effects and conformal symmetries of this model at the critical point. We evaluate the correlation length and the Casimir energy of this model and study their dependence on LL and RR. We examine the modular transformation properties of the partition function, and study the dependence of the specific heat on the mass gap in view of possible extension of the CC-theorem to three dimensions.Comment: 12 pages uuencoded compressed PostScript file including 1 figur

    Ultraviolet Property of Noncommutative Wess-Zumino-Witten Model

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    We construct noncommutative extension of the Wess-Zumino-Witten (WZW) model and study its ultraviolet property. The \beta-function of the U(N) noncommutative WZW model resembles that of the ordinary WZW model. The U(1) noncommutative model has also a nontrivial fixed point.Comment: 7 pages, 1 figur

    Instanton Equations for the Supersymmetric CP^{N-1} Sigma Model on Non(anti)commutative Superspace

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    We study the instanton equation of the supersymmetric CP^{N-1} sigma model on non(anti)commutative superspace in two dimensions. We show that the undeformed instanton equation is consistent with the deformed equations of motion. Then we conclude that the instanton equation is not deformed by superspace non(anti)commutativity.Comment: 6 page

    Vanishing Next-to-Leading Corrections to the \beta-Function of the SUSY CP^{N-1} Model in Three Dimensions

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    We study the ultraviolet properties of the supersymmetric CP^{N-1} sigma model in three dimensions to next-to-leading order in the 1/N expansion. We calculate the \beta-function to this order and verify that it has no next-to-leading order corrections.Comment: 8 pages, 1 figure, the renormalization constant of the field alpha is correcte
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