Lifting of states in 2-dimensional N = 4 supersymmetric CFTs

Abstract We consider states of the D1-D5 CFT where only the left-moving sector is excited. As we deform away from the orbifold point, some of these states will remain BPS while others can ‘lift’. The lifting can be computed by a path integral containing two twist deformations; however, the relevant...

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Main Authors: Bin Guo, Samir D. Mathur
Format: Article
Language:English
Published: SpringerOpen 2019-10-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP10(2019)155
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spelling doaj-d17fea9f47614ec1ab30e5d865592cc92020-11-25T02:25:55ZengSpringerOpenJournal of High Energy Physics1029-84792019-10-0120191014510.1007/JHEP10(2019)155Lifting of states in 2-dimensional N = 4 supersymmetric CFTsBin Guo0Samir D. Mathur1Department of Physics, The Ohio State UniversityDepartment of Physics, The Ohio State UniversityAbstract We consider states of the D1-D5 CFT where only the left-moving sector is excited. As we deform away from the orbifold point, some of these states will remain BPS while others can ‘lift’. The lifting can be computed by a path integral containing two twist deformations; however, the relevant 4-point amplitude cannot be computed explicitly in many cases. We analyze an older proposal by Gava and Narain where the lift can be computed in terms of a finite number of 3-point functions. A direct Hamiltonian decomposition of the path integral involves an infinite number of 3-point functions, as well the first order correction to the starting state. We note that these corrections to the state account for the infinite number of 3-point functions arising from higher energy states, and one can indeed express the path-integral result in terms of a finite number of 3-point functions involving only the leading order states that are degenerate. The first order correction to the super-charge G ¯ 1 $$ {\overline{G}}^{(1)} $$ gets replaced by a projection G ¯ P $$ {\overline{G}}^{(P)} $$ ; this projected operator can also be used to group the states into multiplets whose members have the same lifting.http://link.springer.com/article/10.1007/JHEP10(2019)155Conformal Field TheoryExtended SupersymmetryAdS-CFT Correspondence
collection DOAJ
language English
format Article
sources DOAJ
author Bin Guo
Samir D. Mathur
spellingShingle Bin Guo
Samir D. Mathur
Lifting of states in 2-dimensional N = 4 supersymmetric CFTs
Journal of High Energy Physics
Conformal Field Theory
Extended Supersymmetry
AdS-CFT Correspondence
author_facet Bin Guo
Samir D. Mathur
author_sort Bin Guo
title Lifting of states in 2-dimensional N = 4 supersymmetric CFTs
title_short Lifting of states in 2-dimensional N = 4 supersymmetric CFTs
title_full Lifting of states in 2-dimensional N = 4 supersymmetric CFTs
title_fullStr Lifting of states in 2-dimensional N = 4 supersymmetric CFTs
title_full_unstemmed Lifting of states in 2-dimensional N = 4 supersymmetric CFTs
title_sort lifting of states in 2-dimensional n = 4 supersymmetric cfts
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2019-10-01
description Abstract We consider states of the D1-D5 CFT where only the left-moving sector is excited. As we deform away from the orbifold point, some of these states will remain BPS while others can ‘lift’. The lifting can be computed by a path integral containing two twist deformations; however, the relevant 4-point amplitude cannot be computed explicitly in many cases. We analyze an older proposal by Gava and Narain where the lift can be computed in terms of a finite number of 3-point functions. A direct Hamiltonian decomposition of the path integral involves an infinite number of 3-point functions, as well the first order correction to the starting state. We note that these corrections to the state account for the infinite number of 3-point functions arising from higher energy states, and one can indeed express the path-integral result in terms of a finite number of 3-point functions involving only the leading order states that are degenerate. The first order correction to the super-charge G ¯ 1 $$ {\overline{G}}^{(1)} $$ gets replaced by a projection G ¯ P $$ {\overline{G}}^{(P)} $$ ; this projected operator can also be used to group the states into multiplets whose members have the same lifting.
topic Conformal Field Theory
Extended Supersymmetry
AdS-CFT Correspondence
url http://link.springer.com/article/10.1007/JHEP10(2019)155
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AT samirdmathur liftingofstatesin2dimensionaln4supersymmetriccfts
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