Modular invariance and thermal effective field theory in CFT

Abstract We use thermal effective field theory to derive that the coefficient of the first subleading piece of the thermal free energy, c 1, is equal to the coefficient of the subleading piece of the Casimir energy on S 1 × S d−2 for d ≥ 4. We conjecture that this coefficient obeys a sign constraint...

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Main Authors: Kuroush Allameh, Edgar Shaghoulian
Format: Article
Language:English
Published: SpringerOpen 2025-01-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP01(2025)200
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author Kuroush Allameh
Edgar Shaghoulian
author_facet Kuroush Allameh
Edgar Shaghoulian
author_sort Kuroush Allameh
collection DOAJ
description Abstract We use thermal effective field theory to derive that the coefficient of the first subleading piece of the thermal free energy, c 1, is equal to the coefficient of the subleading piece of the Casimir energy on S 1 × S d−2 for d ≥ 4. We conjecture that this coefficient obeys a sign constraint c 1 ≥ 0 in CFT and collect some evidence for this bound. We discuss various applications of the thermal effective field theory, including placing the CFT on different spatial backgrounds and turning on chemical potentials for U(1) charge and angular momentum. Along the way, we derive the high-temperature partition function on a sphere with arbitrary angular velocities using only time dilation and length contraction.
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spelling doaj-art-52221951c6514a549495bfb3b4e5b62d2025-02-09T12:07:08ZengSpringerOpenJournal of High Energy Physics1029-84792025-01-012025112510.1007/JHEP01(2025)200Modular invariance and thermal effective field theory in CFTKuroush Allameh0Edgar Shaghoulian1Physics Department, UC Santa CruzPhysics Department, UC Santa CruzAbstract We use thermal effective field theory to derive that the coefficient of the first subleading piece of the thermal free energy, c 1, is equal to the coefficient of the subleading piece of the Casimir energy on S 1 × S d−2 for d ≥ 4. We conjecture that this coefficient obeys a sign constraint c 1 ≥ 0 in CFT and collect some evidence for this bound. We discuss various applications of the thermal effective field theory, including placing the CFT on different spatial backgrounds and turning on chemical potentials for U(1) charge and angular momentum. Along the way, we derive the high-temperature partition function on a sphere with arbitrary angular velocities using only time dilation and length contraction.https://doi.org/10.1007/JHEP01(2025)200Conformal and W SymmetryEffective Field TheoriesThermal Field TheoryAdS-CFT Correspondence
spellingShingle Kuroush Allameh
Edgar Shaghoulian
Modular invariance and thermal effective field theory in CFT
Journal of High Energy Physics
Conformal and W Symmetry
Effective Field Theories
Thermal Field Theory
AdS-CFT Correspondence
title Modular invariance and thermal effective field theory in CFT
title_full Modular invariance and thermal effective field theory in CFT
title_fullStr Modular invariance and thermal effective field theory in CFT
title_full_unstemmed Modular invariance and thermal effective field theory in CFT
title_short Modular invariance and thermal effective field theory in CFT
title_sort modular invariance and thermal effective field theory in cft
topic Conformal and W Symmetry
Effective Field Theories
Thermal Field Theory
AdS-CFT Correspondence
url https://doi.org/10.1007/JHEP01(2025)200
work_keys_str_mv AT kuroushallameh modularinvarianceandthermaleffectivefieldtheoryincft
AT edgarshaghoulian modularinvarianceandthermaleffectivefieldtheoryincft