383 research outputs found

    Generalized Gradient Flow Equation and Its Application to Super Yang-Mills Theory

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    We generalize the gradient flow equation for field theories with nonlinearly realized symmetry. Applying the formalism to super Yang-Mills theory, we construct a supersymmetric extension of the gradient flow equation. It can be shown that the super gauge symmetry is preserved in the gradient flow. Furthermore, choosing an appropriate modification term to damp the gauge degrees of freedom, we obtain a gradient flow equation which is closed within the Wess-Zumino gauge.Comment: 35 pages, v2: typos corrected and references added, v3: published versio

    Flow Equation of N=1 Supersymmetric O(N) Nonlinear Sigma Model in Two Dimensions

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    We study the flow equation for the N=1\mathcal{N}=1 supersymmetric O(N)O(N) nonlinear sigma model in two dimensions, which cannot be given by the gradient of the action, as evident from dimensional analysis. Imposing the condition on the flow equation that it respects both the supersymmetry and the O(N)O(N) symmetry, we show that the flow equation has a specific form, which however contains an undetermined function of the supersymmetric derivatives DD and Dˉ\bar D. Taking the most simple choice, we propose a flow equation for this model. As an application of the flow equation, we give the solution of the equation at the leading order in the large NN expansion. The result shows that the flow of the superfield in the model is dominated by the scalar term, since the supersymmetry is unbroken in the original model. It is also shown that the two point function of the superfield is finite at the leading order of the large NN expansion.Comment: 17 pages; v2: published versio

    Geometries from field theories

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    We propose a method to define a d+1d+1 dimensional geometry from a dd dimensional quantum field theory in the 1/N1/N expansion. We first construct a d+1d+1 dimensional field theory from the dd dimensional one via the gradient flow equation, whose flow time tt represents the energy scale of the system such that t0t\rightarrow 0 corresponds to the ultra-violet (UV) while tt\rightarrow\infty to the infra-red (IR). We then define the induced metric from d+1d+1 dimensional field operators. We show that the metric defined in this way becomes classical in the large NN limit, in a sense that quantum fluctuations of the metric are suppressed as 1/N1/N due to the large NN factorization property. As a concrete example, we apply our method to the O(N) non-linear σ\sigma model in two dimensions. We calculate the three dimensional induced metric, which is shown to describe an AdS space in the massless limit. We finally discuss several open issues in future studies.Comment: 9 pages, the title has been changed, and some contents have also been modified. This version is accepted for a publication in PTE

    Commuting difference operators arising from the elliptic C_2^{(1)}-face model

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    We study a pair of commuting difference operators arising from the elliptic C_2^{(1)}-face model. The operators, whose coefficients are expressed in terms of the Jacobi's elliptic theta function, act on the space of meromorphic functions on the weight space of the C_2 type simple Lie algebra. We show that the space of functions spanned by the level one characters of the affine Lie algebra sp(4,C) is invariant under the action of the difference operators.Comment: latex2e file, 19 pages, no figures; added reference

    Gradient Flow of O(N) nonlinear sigma model at large N

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    We study the gradient flow equation for the O(N) nonlinear sigma model in two dimensions at large N. We parameterize solution of the field at flow time t in powers of bare fields by introducing the coefficient function X_n for the n-th power term (n=1,3,...). Reducing the flow equation by keeping only the contributions at leading order in large N, we obtain a set of equations for X_n's, which can be solved iteratively starting from n=1. For n=1 case, we find an explicit form of the exact solution. Using this solution, we show that the two point function at finite flow time t is finite. As an application, we obtain the non-perturbative running coupling defined from the energy density. We also discuss the solution for n=3 case.Comment: 21 pages; v2: minor corrections, added references and note, v3: published versio
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