A surprising similarity between holographic CFTs and a free fermion in (2 + 1) dimensions

Abstract We compare the behavior of the vacuum free energy (i.e. the Casimir energy) of various (2 + 1)-dimensional CFTs on an ultrastatic spacetime as a function of the spatial geometry. The CFTs we consider are a free Dirac fermion, the conformally-coupled scalar, and a holographic CFT, and we tak...

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Main Authors: Krai Cheamsawat, Sebastian Fischetti, Lucas Wallis, Toby Wiseman
Format: Article
Language:English
Published: SpringerOpen 2021-05-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP05(2021)246
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spelling doaj-11d95e2f7a224022b4168b75dee2fb4b2021-05-30T11:07:31ZengSpringerOpenJournal of High Energy Physics1029-84792021-05-012021512410.1007/JHEP05(2021)246A surprising similarity between holographic CFTs and a free fermion in (2 + 1) dimensionsKrai Cheamsawat0Sebastian Fischetti1Lucas Wallis2Toby Wiseman3Theoretical Physics Group, Blackett Laboratory, Imperial CollegeDepartment of Physics, McGill UniversityTheoretical Physics Group, Blackett Laboratory, Imperial CollegeTheoretical Physics Group, Blackett Laboratory, Imperial CollegeAbstract We compare the behavior of the vacuum free energy (i.e. the Casimir energy) of various (2 + 1)-dimensional CFTs on an ultrastatic spacetime as a function of the spatial geometry. The CFTs we consider are a free Dirac fermion, the conformally-coupled scalar, and a holographic CFT, and we take the spatial geometry to be an axisymmetric deformation of the round sphere. The free energies of the fermion and of the scalar are computed numerically using heat kernel methods; the free energy of the holographic CFT is computed numerically from a static, asymptotically AdS dual geometry using a novel approach we introduce here. We find that the free energy of the two free theories is qualitatively similar as a function of the sphere deformation, but we also find that the holographic CFT has a remarkable and mysterious quantitative similarity to the free fermion; this agreement is especially surprising given that the holographic CFT is strongly-coupled. Over the wide ranges of deformations for which we are able to perform the computations accurately, the scalar and fermion differ by up to 50% whereas the holographic CFT differs from the fermion by less than one percent.https://doi.org/10.1007/JHEP05(2021)246AdS-CFT CorrespondenceConformal Field TheoryField Theories in Lower Dimensions
collection DOAJ
language English
format Article
sources DOAJ
author Krai Cheamsawat
Sebastian Fischetti
Lucas Wallis
Toby Wiseman
spellingShingle Krai Cheamsawat
Sebastian Fischetti
Lucas Wallis
Toby Wiseman
A surprising similarity between holographic CFTs and a free fermion in (2 + 1) dimensions
Journal of High Energy Physics
AdS-CFT Correspondence
Conformal Field Theory
Field Theories in Lower Dimensions
author_facet Krai Cheamsawat
Sebastian Fischetti
Lucas Wallis
Toby Wiseman
author_sort Krai Cheamsawat
title A surprising similarity between holographic CFTs and a free fermion in (2 + 1) dimensions
title_short A surprising similarity between holographic CFTs and a free fermion in (2 + 1) dimensions
title_full A surprising similarity between holographic CFTs and a free fermion in (2 + 1) dimensions
title_fullStr A surprising similarity between holographic CFTs and a free fermion in (2 + 1) dimensions
title_full_unstemmed A surprising similarity between holographic CFTs and a free fermion in (2 + 1) dimensions
title_sort surprising similarity between holographic cfts and a free fermion in (2 + 1) dimensions
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-05-01
description Abstract We compare the behavior of the vacuum free energy (i.e. the Casimir energy) of various (2 + 1)-dimensional CFTs on an ultrastatic spacetime as a function of the spatial geometry. The CFTs we consider are a free Dirac fermion, the conformally-coupled scalar, and a holographic CFT, and we take the spatial geometry to be an axisymmetric deformation of the round sphere. The free energies of the fermion and of the scalar are computed numerically using heat kernel methods; the free energy of the holographic CFT is computed numerically from a static, asymptotically AdS dual geometry using a novel approach we introduce here. We find that the free energy of the two free theories is qualitatively similar as a function of the sphere deformation, but we also find that the holographic CFT has a remarkable and mysterious quantitative similarity to the free fermion; this agreement is especially surprising given that the holographic CFT is strongly-coupled. Over the wide ranges of deformations for which we are able to perform the computations accurately, the scalar and fermion differ by up to 50% whereas the holographic CFT differs from the fermion by less than one percent.
topic AdS-CFT Correspondence
Conformal Field Theory
Field Theories in Lower Dimensions
url https://doi.org/10.1007/JHEP05(2021)246
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