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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...
Autores principales: | , , , |
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Lenguaje: | eng |
Publicado: |
2022
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP06(2022)041 http://cds.cern.ch/record/2802827 |
_version_ | 1780972761444777984 |
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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 |
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