Cargando…

The analytic structure of the fixed charge expansion

We investigate the analytic properties of the fixed charge expansion for a number of conformal field theories in different space-time dimensions. The models investigated here are O(N) and QED$_{3}$. We show that in d = 3 − ϵ dimensions the contribution to the O(N) fixed charge Q conformal dimensions...

Descripción completa

Detalles Bibliográficos
Autores principales: Antipin, Oleg, Bersini, Jahmall, Sannino, Francesco, Torres, Matías
Lenguaje:eng
Publicado: 2022
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP06(2022)041
http://cds.cern.ch/record/2802827
_version_ 1780972761444777984
author Antipin, Oleg
Bersini, Jahmall
Sannino, Francesco
Torres, Matías
author_facet Antipin, Oleg
Bersini, Jahmall
Sannino, Francesco
Torres, Matías
author_sort Antipin, Oleg
collection CERN
description We investigate the analytic properties of the fixed charge expansion for a number of conformal field theories in different space-time dimensions. The models investigated here are O(N) and QED$_{3}$. We show that in d = 3 − ϵ dimensions the contribution to the O(N) fixed charge Q conformal dimensions obtained in the double scaling limit of large charge and vanishing ϵ is non-Borel summable, doubly factorial divergent, and with order $ \sqrt{Q} $ optimal truncation order. By using resurgence techniques we show that the singularities in the Borel plane are related to worldline instantons that were discovered in the other double scaling limit of large Q and N of ref. [1]. In d = 4 − ϵ dimensions the story changes since in the same large Q and small E regime the next order corrections to the scaling dimensions lead to a convergent series. The resummed series displays a new branch cut singularity which is relevant for the stability of the O(N) large charge sector for negative ϵ. Although the QED$_{3}$ model shares the same large charge behaviour of the O(N) model, we discover that at leading order in the large number of matter field expansion the large charge scaling dimensions are Borel summable, single factorial divergent, and with order Q optimal truncation order.
id cern-2802827
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2022
record_format invenio
spelling cern-28028272023-10-04T06:50:14Zdoi:10.1007/JHEP06(2022)041http://cds.cern.ch/record/2802827engAntipin, OlegBersini, JahmallSannino, FrancescoTorres, MatíasThe analytic structure of the fixed charge expansionhep-phParticle Physics - Phenomenologycond-mat.stat-mechhep-thParticle Physics - TheoryWe investigate the analytic properties of the fixed charge expansion for a number of conformal field theories in different space-time dimensions. The models investigated here are O(N) and QED$_{3}$. We show that in d = 3 − ϵ dimensions the contribution to the O(N) fixed charge Q conformal dimensions obtained in the double scaling limit of large charge and vanishing ϵ is non-Borel summable, doubly factorial divergent, and with order $ \sqrt{Q} $ optimal truncation order. By using resurgence techniques we show that the singularities in the Borel plane are related to worldline instantons that were discovered in the other double scaling limit of large Q and N of ref. [1]. In d = 4 − ϵ dimensions the story changes since in the same large Q and small E regime the next order corrections to the scaling dimensions lead to a convergent series. The resummed series displays a new branch cut singularity which is relevant for the stability of the O(N) large charge sector for negative ϵ. Although the QED$_{3}$ model shares the same large charge behaviour of the O(N) model, we discover that at leading order in the large number of matter field expansion the large charge scaling dimensions are Borel summable, single factorial divergent, and with order Q optimal truncation order.We investigate the analytic properties of the fixed charge expansion for a number of conformal field theories in different space-time dimensions. The models investigated here are $O(N)$ and $QED_3$. We show that in $d=3-\epsilon$ dimensions the contribution to the $O(N)$ fixed charge $Q$ conformal dimensions obtained in the double scaling limit of large charge and vanishing $\epsilon$ is non-Borel summable, doubly factorial divergent, and with order $\sqrt{Q}$ optimal truncation order. By using resurgence techniques we show that the singularities in the Borel plane are related to worldline instantons that were discovered in the other double scaling limit of large $Q$ and $N$ of Ref. [1]. In $d=4-\epsilon$ dimensions the story changes since in the same large $Q$ and small $\epsilon$ regime the next order corrections to the scaling dimensions lead to a convergent series. The resummed series displays a new branch cut singularity which is relevant for the stability of the $O(N)$ large charge sector for negative $\epsilon$. Although the $QED_3$ model shares the same large charge behaviour of the $O(N)$ model, we discover that at leading order in the large number of matter field expansion the large charge scaling dimensions are Borel summable, single factorial divergent, and with order $Q$ optimal truncation order.arXiv:2202.13165RBI-ThPhys-2022-6CERN-TH-2022-049oai:cds.cern.ch:28028272022-02-26
spellingShingle hep-ph
Particle Physics - Phenomenology
cond-mat.stat-mech
hep-th
Particle Physics - Theory
Antipin, Oleg
Bersini, Jahmall
Sannino, Francesco
Torres, Matías
The analytic structure of the fixed charge expansion
title The analytic structure of the fixed charge expansion
title_full The analytic structure of the fixed charge expansion
title_fullStr The analytic structure of the fixed charge expansion
title_full_unstemmed The analytic structure of the fixed charge expansion
title_short The analytic structure of the fixed charge expansion
title_sort analytic structure of the fixed charge expansion
topic hep-ph
Particle Physics - Phenomenology
cond-mat.stat-mech
hep-th
Particle Physics - Theory
url https://dx.doi.org/10.1007/JHEP06(2022)041
http://cds.cern.ch/record/2802827
work_keys_str_mv AT antipinoleg theanalyticstructureofthefixedchargeexpansion
AT bersinijahmall theanalyticstructureofthefixedchargeexpansion
AT sanninofrancesco theanalyticstructureofthefixedchargeexpansion
AT torresmatias theanalyticstructureofthefixedchargeexpansion
AT antipinoleg analyticstructureofthefixedchargeexpansion
AT bersinijahmall analyticstructureofthefixedchargeexpansion
AT sanninofrancesco analyticstructureofthefixedchargeexpansion
AT torresmatias analyticstructureofthefixedchargeexpansion