The quark anti-quark potential and the cusp anomalous dimension from a TBA equation
- Autores
- Correa, Diego Hernán; Maldacena, Juan M.; Sever, Amit
- Año de publicación
- 2012
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- We derive a set of integral equations of the TBA type for the generalized cusp anomalous dimension, or the quark antiquark potential on the three sphere, as a function of the angles. We do this by considering a family of local operators on a Wilson loop with charge L. In the large L limit the problem can be solved in terms of a certain boundary reflection matrix. We determine this reflection matrix by using the symmetries and the boundary crossing equation. The cusp is introduced through a relative rotation between the two boundaries. Then the TBA trick of exchanging space and time leads to an exact equation for all values of L. The L = 0 case corresponds to the cusped Wilson loop with no operators inserted. We then derive a slightly simplified integral equation which describes the small angle limit. We solve this equation up to three loops in perturbation theory and match the results that were obtained with more direct approaches.
Instituto de Física La Plata - Materia
-
Ciencias Exactas
Hooft and Polyakov loops
Scattering amplitudes
Wilson
Integrable field theories
AdS-CFT Correspondence - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- http://creativecommons.org/licenses/by-nc-sa/2.5/ar/
- Repositorio
- Institución
- Universidad Nacional de La Plata
- OAI Identificador
- oai:sedici.unlp.edu.ar:10915/96169
Ver los metadatos del registro completo
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The quark anti-quark potential and the cusp anomalous dimension from a TBA equationCorrea, Diego HernánMaldacena, Juan M.Sever, AmitCiencias ExactasHooft and Polyakov loopsScattering amplitudesWilsonIntegrable field theoriesAdS-CFT CorrespondenceWe derive a set of integral equations of the TBA type for the generalized cusp anomalous dimension, or the quark antiquark potential on the three sphere, as a function of the angles. We do this by considering a family of local operators on a Wilson loop with charge L. In the large L limit the problem can be solved in terms of a certain boundary reflection matrix. We determine this reflection matrix by using the symmetries and the boundary crossing equation. The cusp is introduced through a relative rotation between the two boundaries. Then the TBA trick of exchanging space and time leads to an exact equation for all values of L. The L = 0 case corresponds to the cusped Wilson loop with no operators inserted. We then derive a slightly simplified integral equation which describes the small angle limit. We solve this equation up to three loops in perturbation theory and match the results that were obtained with more direct approaches.Instituto de Física La Plata2012-08-28info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfhttp://sedici.unlp.edu.ar/handle/10915/96169enginfo:eu-repo/semantics/altIdentifier/url/https://ri.conicet.gov.ar/11336/75091info:eu-repo/semantics/altIdentifier/url/https://link.springer.com/article/10.1007%2FJHEP08%282012%29134info:eu-repo/semantics/altIdentifier/issn/1126-6708info:eu-repo/semantics/altIdentifier/doi/10.1007/JHEP08(2012)134info:eu-repo/semantics/altIdentifier/hdl/11336/75091info:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-sa/2.5/ar/Creative Commons Attribution-NonCommercial-ShareAlike 2.5 Argentina (CC BY-NC-SA 2.5)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-09-03T10:52:37Zoai:sedici.unlp.edu.ar:10915/96169Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-09-03 10:52:37.301SEDICI (UNLP) - Universidad Nacional de La Platafalse |
dc.title.none.fl_str_mv |
The quark anti-quark potential and the cusp anomalous dimension from a TBA equation |
title |
The quark anti-quark potential and the cusp anomalous dimension from a TBA equation |
spellingShingle |
The quark anti-quark potential and the cusp anomalous dimension from a TBA equation Correa, Diego Hernán Ciencias Exactas Hooft and Polyakov loops Scattering amplitudes Wilson Integrable field theories AdS-CFT Correspondence |
title_short |
The quark anti-quark potential and the cusp anomalous dimension from a TBA equation |
title_full |
The quark anti-quark potential and the cusp anomalous dimension from a TBA equation |
title_fullStr |
The quark anti-quark potential and the cusp anomalous dimension from a TBA equation |
title_full_unstemmed |
The quark anti-quark potential and the cusp anomalous dimension from a TBA equation |
title_sort |
The quark anti-quark potential and the cusp anomalous dimension from a TBA equation |
dc.creator.none.fl_str_mv |
Correa, Diego Hernán Maldacena, Juan M. Sever, Amit |
author |
Correa, Diego Hernán |
author_facet |
Correa, Diego Hernán Maldacena, Juan M. Sever, Amit |
author_role |
author |
author2 |
Maldacena, Juan M. Sever, Amit |
author2_role |
author author |
dc.subject.none.fl_str_mv |
Ciencias Exactas Hooft and Polyakov loops Scattering amplitudes Wilson Integrable field theories AdS-CFT Correspondence |
topic |
Ciencias Exactas Hooft and Polyakov loops Scattering amplitudes Wilson Integrable field theories AdS-CFT Correspondence |
dc.description.none.fl_txt_mv |
We derive a set of integral equations of the TBA type for the generalized cusp anomalous dimension, or the quark antiquark potential on the three sphere, as a function of the angles. We do this by considering a family of local operators on a Wilson loop with charge L. In the large L limit the problem can be solved in terms of a certain boundary reflection matrix. We determine this reflection matrix by using the symmetries and the boundary crossing equation. The cusp is introduced through a relative rotation between the two boundaries. Then the TBA trick of exchanging space and time leads to an exact equation for all values of L. The L = 0 case corresponds to the cusped Wilson loop with no operators inserted. We then derive a slightly simplified integral equation which describes the small angle limit. We solve this equation up to three loops in perturbation theory and match the results that were obtained with more direct approaches. Instituto de Física La Plata |
description |
We derive a set of integral equations of the TBA type for the generalized cusp anomalous dimension, or the quark antiquark potential on the three sphere, as a function of the angles. We do this by considering a family of local operators on a Wilson loop with charge L. In the large L limit the problem can be solved in terms of a certain boundary reflection matrix. We determine this reflection matrix by using the symmetries and the boundary crossing equation. The cusp is introduced through a relative rotation between the two boundaries. Then the TBA trick of exchanging space and time leads to an exact equation for all values of L. The L = 0 case corresponds to the cusped Wilson loop with no operators inserted. We then derive a slightly simplified integral equation which describes the small angle limit. We solve this equation up to three loops in perturbation theory and match the results that were obtained with more direct approaches. |
publishDate |
2012 |
dc.date.none.fl_str_mv |
2012-08-28 |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion Articulo http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
format |
article |
status_str |
publishedVersion |
dc.identifier.none.fl_str_mv |
http://sedici.unlp.edu.ar/handle/10915/96169 |
url |
http://sedici.unlp.edu.ar/handle/10915/96169 |
dc.language.none.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
info:eu-repo/semantics/altIdentifier/url/https://ri.conicet.gov.ar/11336/75091 info:eu-repo/semantics/altIdentifier/url/https://link.springer.com/article/10.1007%2FJHEP08%282012%29134 info:eu-repo/semantics/altIdentifier/issn/1126-6708 info:eu-repo/semantics/altIdentifier/doi/10.1007/JHEP08(2012)134 info:eu-repo/semantics/altIdentifier/hdl/11336/75091 |
dc.rights.none.fl_str_mv |
info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by-nc-sa/2.5/ar/ Creative Commons Attribution-NonCommercial-ShareAlike 2.5 Argentina (CC BY-NC-SA 2.5) |
eu_rights_str_mv |
openAccess |
rights_invalid_str_mv |
http://creativecommons.org/licenses/by-nc-sa/2.5/ar/ Creative Commons Attribution-NonCommercial-ShareAlike 2.5 Argentina (CC BY-NC-SA 2.5) |
dc.format.none.fl_str_mv |
application/pdf |
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reponame:SEDICI (UNLP) instname:Universidad Nacional de La Plata instacron:UNLP |
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Universidad Nacional de La Plata |
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SEDICI (UNLP) - Universidad Nacional de La Plata |
repository.mail.fl_str_mv |
alira@sedici.unlp.edu.ar |
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