Gradient Properties of Perturbative Multiscalar RG Flows to Six Loops

Fuente: arXiv
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Main Authors: Pannell, William H., Stergiou, Andreas
Format: Preprint
Published: 2024
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author Pannell, William H.
Stergiou, Andreas
author_facet Pannell, William H.
Stergiou, Andreas
contents The gradient property of the renormalisation group (RG) flow of multiscalar theories is examined perturbatively in $d=4$ and $d=4-\varepsilon$ dimensions. Such theories undergo RG flows in the space of quartic couplings $λ^I$. Starting at five loops, the relevant vector field that determines the physical RG flow is not the beta function traditionally computed in a minimal subtraction scheme in dimensional regularisation, but a suitable modification of it, the $B$ function. It is found that up to five loops the $B$ vector field is gradient, i.e. $B^I=G^{IJ}\partial A / \partialλ^J$ with $A$ a scalar and $G_{IJ}$ a rank-two symmetric tensor of the couplings. Up to five loops the beta function is also gradient, but it fails to be so at six loops. The conditions under which the $B$ function (and hence the RG flow) is gradient at six loops are specified, but their verification rests on a separate six-loop computation that remains to be performed.
format Preprint
id arxiv_https___arxiv_org_abs_2402_17817
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Gradient Properties of Perturbative Multiscalar RG Flows to Six Loops
Pannell, William H.
Stergiou, Andreas
High Energy Physics - Theory
Statistical Mechanics
High Energy Physics - Phenomenology
The gradient property of the renormalisation group (RG) flow of multiscalar theories is examined perturbatively in $d=4$ and $d=4-\varepsilon$ dimensions. Such theories undergo RG flows in the space of quartic couplings $λ^I$. Starting at five loops, the relevant vector field that determines the physical RG flow is not the beta function traditionally computed in a minimal subtraction scheme in dimensional regularisation, but a suitable modification of it, the $B$ function. It is found that up to five loops the $B$ vector field is gradient, i.e. $B^I=G^{IJ}\partial A / \partialλ^J$ with $A$ a scalar and $G_{IJ}$ a rank-two symmetric tensor of the couplings. Up to five loops the beta function is also gradient, but it fails to be so at six loops. The conditions under which the $B$ function (and hence the RG flow) is gradient at six loops are specified, but their verification rests on a separate six-loop computation that remains to be performed.
title Gradient Properties of Perturbative Multiscalar RG Flows to Six Loops
topic High Energy Physics - Theory
Statistical Mechanics
High Energy Physics - Phenomenology
url https://arxiv.org/abs/2402.17817