Holographic RG flows on curved manifolds and the F-theorem

Abstract We study F-functions in the context of field theories on S 3 using gauge-gravity duality, with the radius of S 3 playing the role of RG scale. We show that the on-shell action, evaluated over a set of holographic RG flow solutions, can be used to define good F-functions, which decrease mono...

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Main Authors: J. K. Ghosh, E. Kiritsis, F. Nitti, L. T. Witkowski
Format: Article
Language:English
Published: SpringerOpen 2019-02-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP02(2019)055
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spelling doaj-6b2206a34eb24d91b301b3da42afb8342020-11-25T01:21:50ZengSpringerOpenJournal of High Energy Physics1029-84792019-02-012019218610.1007/JHEP02(2019)055Holographic RG flows on curved manifolds and the F-theoremJ. K. Ghosh0E. Kiritsis1F. Nitti2L. T. Witkowski3APC, AstroParticule et Cosmologie, Université Paris Diderot, CNRS/IN2P3, CEA/IRFU, Observatoire de Paris, Sorbonne Paris CitéAPC, AstroParticule et Cosmologie, Université Paris Diderot, CNRS/IN2P3, CEA/IRFU, Observatoire de Paris, Sorbonne Paris CitéAPC, AstroParticule et Cosmologie, Université Paris Diderot, CNRS/IN2P3, CEA/IRFU, Observatoire de Paris, Sorbonne Paris CitéAPC, AstroParticule et Cosmologie, Université Paris Diderot, CNRS/IN2P3, CEA/IRFU, Observatoire de Paris, Sorbonne Paris CitéAbstract We study F-functions in the context of field theories on S 3 using gauge-gravity duality, with the radius of S 3 playing the role of RG scale. We show that the on-shell action, evaluated over a set of holographic RG flow solutions, can be used to define good F-functions, which decrease monotonically along the RG flow from the UV to the IR for a wide range of examples. If the operator perturbing the UV CFT has dimension Δ > 3/2 these F -functions correspond to an appropriately renormalized free energy. If instead the perturbing operator has dimension Δ < 3/2 it is the quantum effective potential, i.e. the Legendre transform of the free energy, which gives rise to good F-functions. We check that these observations hold beyond holography for the case of a free fermion on S 3 (Δ = 2) and the free boson on S 3 (Δ = 1), resolving a long-standing problem regarding the non-monotonicity of the free energy for the free massive scalar. We also show that for a particular choice of entangling surface, we can define good F-functions from an entanglement entropy, which coincide with certain F-functions obtained from the on-shell action.http://link.springer.com/article/10.1007/JHEP02(2019)055AdS-CFT CorrespondenceRenormalization Group
collection DOAJ
language English
format Article
sources DOAJ
author J. K. Ghosh
E. Kiritsis
F. Nitti
L. T. Witkowski
spellingShingle J. K. Ghosh
E. Kiritsis
F. Nitti
L. T. Witkowski
Holographic RG flows on curved manifolds and the F-theorem
Journal of High Energy Physics
AdS-CFT Correspondence
Renormalization Group
author_facet J. K. Ghosh
E. Kiritsis
F. Nitti
L. T. Witkowski
author_sort J. K. Ghosh
title Holographic RG flows on curved manifolds and the F-theorem
title_short Holographic RG flows on curved manifolds and the F-theorem
title_full Holographic RG flows on curved manifolds and the F-theorem
title_fullStr Holographic RG flows on curved manifolds and the F-theorem
title_full_unstemmed Holographic RG flows on curved manifolds and the F-theorem
title_sort holographic rg flows on curved manifolds and the f-theorem
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-02-01
description Abstract We study F-functions in the context of field theories on S 3 using gauge-gravity duality, with the radius of S 3 playing the role of RG scale. We show that the on-shell action, evaluated over a set of holographic RG flow solutions, can be used to define good F-functions, which decrease monotonically along the RG flow from the UV to the IR for a wide range of examples. If the operator perturbing the UV CFT has dimension Δ > 3/2 these F -functions correspond to an appropriately renormalized free energy. If instead the perturbing operator has dimension Δ < 3/2 it is the quantum effective potential, i.e. the Legendre transform of the free energy, which gives rise to good F-functions. We check that these observations hold beyond holography for the case of a free fermion on S 3 (Δ = 2) and the free boson on S 3 (Δ = 1), resolving a long-standing problem regarding the non-monotonicity of the free energy for the free massive scalar. We also show that for a particular choice of entangling surface, we can define good F-functions from an entanglement entropy, which coincide with certain F-functions obtained from the on-shell action.
topic AdS-CFT Correspondence
Renormalization Group
url http://link.springer.com/article/10.1007/JHEP02(2019)055
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AT ekiritsis holographicrgflowsoncurvedmanifoldsandtheftheorem
AT fnitti holographicrgflowsoncurvedmanifoldsandtheftheorem
AT ltwitkowski holographicrgflowsoncurvedmanifoldsandtheftheorem
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