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Geometric Derivation of the Finite $N$ Master Loop Equation
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abstract
In this paper we provide a geometric derivation of the master loop equation for the lattice Yang-Mills model with structure group $G \in \{SO(N),SU(N), U(N)\}$. This approach is based on integration by parts on $G$. In the appendix we compare our approach to that of \cite{Ch19a} and \cite{J16} based on Schwinger-Dyson equations, and \cite{SheSmZh22} based on stochastic analysis. In particular these approaches are all easily seen to be equivalent. The novelty in our approach is the use of intrinsic geometry of $G$ which we believe simplifies the derivation.
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Cited by 1 Pith paper
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Makeenko-Migdal equations for 2D Yang-Mills: from lattice to continuum
Suitable linear combinations of the discrete Makeenko-Migdal loop equations on (εZ)^2 converge to the continuum Makeenko-Migdal equation on the plane for U(N), SU(N), and SO(N).
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