Analyticity of critical exponents of the $O(N)$ models from nonperturbative renormalization

We employ the functional renormalization group framework at the second order in the derivative expansion to study the $O(N)$ models continuously varying the number of field components $N$ and the spatial dimensionality $d$. We in particular address the Cardy-Hamber prediction concerning nonanalytic...

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Main Author: Andrzej Chlebicki, Pawel Jakubczyk
Format: Article
Language:English
Published: SciPost 2021-06-01
Series:SciPost Physics
Online Access:https://scipost.org/SciPostPhys.10.6.134
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spelling doaj-c897a80f48e542abb3fb3a99be1a797c2021-06-07T10:40:19ZengSciPostSciPost Physics2542-46532021-06-0110613410.21468/SciPostPhys.10.6.134Analyticity of critical exponents of the $O(N)$ models from nonperturbative renormalizationAndrzej Chlebicki, Pawel JakubczykWe employ the functional renormalization group framework at the second order in the derivative expansion to study the $O(N)$ models continuously varying the number of field components $N$ and the spatial dimensionality $d$. We in particular address the Cardy-Hamber prediction concerning nonanalytical behavior of the critical exponents $\nu$ and $\eta$ across a line in the $(d,N)$ plane, which passes through the point $(2,2)$. By direct numerical evaluation of $\eta(d,N)$ and $\nu^{-1}(d,N)$ as well as analysis of the functional fixed-point profiles, we find clear indications of this line in the form of a crossover between two regimes in the $(d,N)$ plane, however no evidence of discontinuous or singular first and second derivatives of these functions for $d>2$. The computed derivatives of $\eta(d,N)$ and $\nu^{-1}(d,N)$ become increasingly large for $d\to 2$ and $N\to 2$ and it is only in this limit that $\eta(d,N)$ and $\nu^{-1}(d,N)$ as obtained by us are evidently nonanalytical. By scanning the dependence of the subleading eigenvalue of the RG transformation on $N$ for $d>2$ we find no indication of its vanishing as anticipated by the Cardy-Hamber scenario. For dimensionality $d$ approaching 3 there are no signatures of the Cardy-Hamber line even as a crossover and its existence in the form of a nonanalyticity of the anticipated form is excluded.https://scipost.org/SciPostPhys.10.6.134
collection DOAJ
language English
format Article
sources DOAJ
author Andrzej Chlebicki, Pawel Jakubczyk
spellingShingle Andrzej Chlebicki, Pawel Jakubczyk
Analyticity of critical exponents of the $O(N)$ models from nonperturbative renormalization
SciPost Physics
author_facet Andrzej Chlebicki, Pawel Jakubczyk
author_sort Andrzej Chlebicki, Pawel Jakubczyk
title Analyticity of critical exponents of the $O(N)$ models from nonperturbative renormalization
title_short Analyticity of critical exponents of the $O(N)$ models from nonperturbative renormalization
title_full Analyticity of critical exponents of the $O(N)$ models from nonperturbative renormalization
title_fullStr Analyticity of critical exponents of the $O(N)$ models from nonperturbative renormalization
title_full_unstemmed Analyticity of critical exponents of the $O(N)$ models from nonperturbative renormalization
title_sort analyticity of critical exponents of the $o(n)$ models from nonperturbative renormalization
publisher SciPost
series SciPost Physics
issn 2542-4653
publishDate 2021-06-01
description We employ the functional renormalization group framework at the second order in the derivative expansion to study the $O(N)$ models continuously varying the number of field components $N$ and the spatial dimensionality $d$. We in particular address the Cardy-Hamber prediction concerning nonanalytical behavior of the critical exponents $\nu$ and $\eta$ across a line in the $(d,N)$ plane, which passes through the point $(2,2)$. By direct numerical evaluation of $\eta(d,N)$ and $\nu^{-1}(d,N)$ as well as analysis of the functional fixed-point profiles, we find clear indications of this line in the form of a crossover between two regimes in the $(d,N)$ plane, however no evidence of discontinuous or singular first and second derivatives of these functions for $d>2$. The computed derivatives of $\eta(d,N)$ and $\nu^{-1}(d,N)$ become increasingly large for $d\to 2$ and $N\to 2$ and it is only in this limit that $\eta(d,N)$ and $\nu^{-1}(d,N)$ as obtained by us are evidently nonanalytical. By scanning the dependence of the subleading eigenvalue of the RG transformation on $N$ for $d>2$ we find no indication of its vanishing as anticipated by the Cardy-Hamber scenario. For dimensionality $d$ approaching 3 there are no signatures of the Cardy-Hamber line even as a crossover and its existence in the form of a nonanalyticity of the anticipated form is excluded.
url https://scipost.org/SciPostPhys.10.6.134
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