Gradient properties of 3 in d=6-

Abstract

The renormalization group flow of the multiscalar interacting 3 theory in d=6 dimensions is known to have a gradient structure, in which suitable generalizations of the beta functions BI emerge as the gradient of a scalar function A, ∂I A = TIJ BJ , with a nontrivial tensor TIJ in the space of couplings. This has been shown directly to three loops in schemes such as MS and can be argued in general by identifying A with the coefficient of the topological term of the trace-anomaly in d=6 up to a normalization. In this paper we show that the same renormalization group has a gradient structure in d=6-. The requirement of a gradient structure is translated to linear constraints that the coefficients of the MS beta functions must obey, one of which is new and pertinent only to the extension to d ≠ 6.

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