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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Online Access: | http://link.springer.com/article/10.1007/JHEP10(2019)155 |
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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 |
work_keys_str_mv |
AT binguo liftingofstatesin2dimensionaln4supersymmetriccfts AT samirdmathur liftingofstatesin2dimensionaln4supersymmetriccfts |
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