Wilson surface central charge from holographic entanglement entropy

Abstract We use entanglement entropy to define a central charge associated to a twodimensional defect or boundary in a conformal field theory (CFT). We present holographic calculations of this central charge for several maximally supersymmetric CFTs dual to eleven-dimensional supergravity in Anti-de...

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Main Authors: John Estes, Darya Krym, Andy O’Bannon, Brandon Robinson, Ronnie Rodgers
Format: Article
Language:English
Published: SpringerOpen 2019-05-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP05(2019)032
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spelling doaj-76962f6b301e4097a9f0908bf41577c92020-11-25T02:55:17ZengSpringerOpenJournal of High Energy Physics1029-84792019-05-012019515310.1007/JHEP05(2019)032Wilson surface central charge from holographic entanglement entropyJohn Estes0Darya Krym1Andy O’Bannon2Brandon Robinson3Ronnie Rodgers4New York City College of Technology, City University of New YorkNew York City College of Technology, City University of New YorkSTAG Research Centre, Physics and Astronomy, University of SouthamptonSTAG Research Centre, Physics and Astronomy, University of SouthamptonSTAG Research Centre, Physics and Astronomy, University of SouthamptonAbstract We use entanglement entropy to define a central charge associated to a twodimensional defect or boundary in a conformal field theory (CFT). We present holographic calculations of this central charge for several maximally supersymmetric CFTs dual to eleven-dimensional supergravity in Anti-de Sitter space, namely the M5-brane theory with a Wilson surface defect and three-dimensional CFTs related to the M2-brane theory with a boundary. Our results for the central charge depend on a partition of N M2-branes ending on M M5-branes. For the Wilson surface, the partition specifies a representation of the gauge algebra, and we write our result for the central charge in a compact form in terms of the algebra’s Weyl vector and the representation’s highest weight vector. We explore how the central charge scales with N and M for some examples of partitions. In general the central charge does not scale as M 3 or N 3/2, the number of degrees of freedom of the M5- or M2-brane theory at large M or N , respectively.http://link.springer.com/article/10.1007/JHEP05(2019)032AdS-CFT CorrespondenceGauge-gravity correspondenceM-Theoryp-branes
collection DOAJ
language English
format Article
sources DOAJ
author John Estes
Darya Krym
Andy O’Bannon
Brandon Robinson
Ronnie Rodgers
spellingShingle John Estes
Darya Krym
Andy O’Bannon
Brandon Robinson
Ronnie Rodgers
Wilson surface central charge from holographic entanglement entropy
Journal of High Energy Physics
AdS-CFT Correspondence
Gauge-gravity correspondence
M-Theory
p-branes
author_facet John Estes
Darya Krym
Andy O’Bannon
Brandon Robinson
Ronnie Rodgers
author_sort John Estes
title Wilson surface central charge from holographic entanglement entropy
title_short Wilson surface central charge from holographic entanglement entropy
title_full Wilson surface central charge from holographic entanglement entropy
title_fullStr Wilson surface central charge from holographic entanglement entropy
title_full_unstemmed Wilson surface central charge from holographic entanglement entropy
title_sort wilson surface central charge from holographic entanglement entropy
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-05-01
description Abstract We use entanglement entropy to define a central charge associated to a twodimensional defect or boundary in a conformal field theory (CFT). We present holographic calculations of this central charge for several maximally supersymmetric CFTs dual to eleven-dimensional supergravity in Anti-de Sitter space, namely the M5-brane theory with a Wilson surface defect and three-dimensional CFTs related to the M2-brane theory with a boundary. Our results for the central charge depend on a partition of N M2-branes ending on M M5-branes. For the Wilson surface, the partition specifies a representation of the gauge algebra, and we write our result for the central charge in a compact form in terms of the algebra’s Weyl vector and the representation’s highest weight vector. We explore how the central charge scales with N and M for some examples of partitions. In general the central charge does not scale as M 3 or N 3/2, the number of degrees of freedom of the M5- or M2-brane theory at large M or N , respectively.
topic AdS-CFT Correspondence
Gauge-gravity correspondence
M-Theory
p-branes
url http://link.springer.com/article/10.1007/JHEP05(2019)032
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