On the dynamics of protected ramond ground states in the D1-D5 CFT

Abstract We examine the behavior of the Ramond ground states in the D1-D5 CFT after a deformation of the free-orbifold sigma model on target space ( T 4 $$ {\mathbbm{T}}^4 $$ ) N /S N by a marginal interaction operator. These states are compositions of Ramond ground states of the twisted and untwist...

Full description

Bibliographic Details
Main Authors: A. A. Lima, G. M. Sotkov, M. Stanishkov
Format: Article
Language:English
Published: SpringerOpen 2021-07-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP07(2021)120
_version_ 1818455154822742016
author A. A. Lima
G. M. Sotkov
M. Stanishkov
author_facet A. A. Lima
G. M. Sotkov
M. Stanishkov
author_sort A. A. Lima
collection DOAJ
description Abstract We examine the behavior of the Ramond ground states in the D1-D5 CFT after a deformation of the free-orbifold sigma model on target space ( T 4 $$ {\mathbbm{T}}^4 $$ ) N /S N by a marginal interaction operator. These states are compositions of Ramond ground states of the twisted and untwisted sectors. They are characterized by a conjugacy class of S N and by the set of their “spins”, including both R-charge and “internal” SU(2) charge. We compute the four-point functions of an arbitrary Ramond ground state with its conjugate and two interaction operators, for genus-zero covering surfaces representing the leading orders in the large-N expansion. We examine short distance limits of these four-point functions, shedding light on the dynamics of the interacting theory. We find the OPEs and a collection of structure constants of the ground states with the interaction operators and a set of resulting non-BPS twisted operators. We also calculate the integrals of the four-point functions over the positions of the interaction operators and show that they vanish. This provides an explicit demonstration that the Ramond ground states remain protected against deformations away of the free orbifold point, as expected from algebraic considerations using the spectral flow of the N $$ \mathcal{N} $$ = (4, 4) superconformal algebra with central charge c = 6N.
first_indexed 2024-12-14T22:06:16Z
format Article
id doaj.art-1658ee9cb52a43b09a16d16ce692d649
institution Directory Open Access Journal
issn 1029-8479
language English
last_indexed 2024-12-14T22:06:16Z
publishDate 2021-07-01
publisher SpringerOpen
record_format Article
series Journal of High Energy Physics
spelling doaj.art-1658ee9cb52a43b09a16d16ce692d6492022-12-21T22:45:52ZengSpringerOpenJournal of High Energy Physics1029-84792021-07-012021714510.1007/JHEP07(2021)120On the dynamics of protected ramond ground states in the D1-D5 CFTA. A. Lima0G. M. Sotkov1M. Stanishkov2Department of Physics, Federal University of Espírito SantoDepartment of Physics, Federal University of Espírito SantoInstitute for Nuclear Research and Nuclear Energy, Bulgarian Academy of SciencesAbstract We examine the behavior of the Ramond ground states in the D1-D5 CFT after a deformation of the free-orbifold sigma model on target space ( T 4 $$ {\mathbbm{T}}^4 $$ ) N /S N by a marginal interaction operator. These states are compositions of Ramond ground states of the twisted and untwisted sectors. They are characterized by a conjugacy class of S N and by the set of their “spins”, including both R-charge and “internal” SU(2) charge. We compute the four-point functions of an arbitrary Ramond ground state with its conjugate and two interaction operators, for genus-zero covering surfaces representing the leading orders in the large-N expansion. We examine short distance limits of these four-point functions, shedding light on the dynamics of the interacting theory. We find the OPEs and a collection of structure constants of the ground states with the interaction operators and a set of resulting non-BPS twisted operators. We also calculate the integrals of the four-point functions over the positions of the interaction operators and show that they vanish. This provides an explicit demonstration that the Ramond ground states remain protected against deformations away of the free orbifold point, as expected from algebraic considerations using the spectral flow of the N $$ \mathcal{N} $$ = (4, 4) superconformal algebra with central charge c = 6N.https://doi.org/10.1007/JHEP07(2021)120Conformal Field TheoryConformal Field Models in String Theory
spellingShingle A. A. Lima
G. M. Sotkov
M. Stanishkov
On the dynamics of protected ramond ground states in the D1-D5 CFT
Journal of High Energy Physics
Conformal Field Theory
Conformal Field Models in String Theory
title On the dynamics of protected ramond ground states in the D1-D5 CFT
title_full On the dynamics of protected ramond ground states in the D1-D5 CFT
title_fullStr On the dynamics of protected ramond ground states in the D1-D5 CFT
title_full_unstemmed On the dynamics of protected ramond ground states in the D1-D5 CFT
title_short On the dynamics of protected ramond ground states in the D1-D5 CFT
title_sort on the dynamics of protected ramond ground states in the d1 d5 cft
topic Conformal Field Theory
Conformal Field Models in String Theory
url https://doi.org/10.1007/JHEP07(2021)120
work_keys_str_mv AT aalima onthedynamicsofprotectedramondgroundstatesinthed1d5cft
AT gmsotkov onthedynamicsofprotectedramondgroundstatesinthed1d5cft
AT mstanishkov onthedynamicsofprotectedramondgroundstatesinthed1d5cft