The Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order

We complete the computation of the Mueller-Tang jet impact factor at next-to-leading order (NLO) initiated in arXiv:1406.5625 and presented in arXiv:1404.2937 by computing the real corrections associated to gluons in the initial state making use of Lipatov's effective action. NLO corrections fo...

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Detalles Bibliográficos
Autores principales: Hentschinski, Martin, Martínez, José Daniel Madrigal, Murdaca, Beatrice, Sabio Vera, Agustín
Lenguaje:eng
Publicado: 2014
Materias:
Particle Physics - Phenomenology
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2014.10.026
http://cds.cern.ch/record/1950179
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author Hentschinski, Martin
Martínez, José Daniel Madrigal
Murdaca, Beatrice
Sabio Vera, Agustín
author_facet Hentschinski, Martin
Martínez, José Daniel Madrigal
Murdaca, Beatrice
Sabio Vera, Agustín
author_sort Hentschinski, Martin
collection CERN
description We complete the computation of the Mueller-Tang jet impact factor at next-to-leading order (NLO) initiated in arXiv:1406.5625 and presented in arXiv:1404.2937 by computing the real corrections associated to gluons in the initial state making use of Lipatov's effective action. NLO corrections for this effective vertex are an important ingredient for a reliable description of large rapidity gap phenomenology within the BFKL approach.
id cern-1950179
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2014
record_format invenio
spelling cern-19501792023-10-04T05:57:52Zdoi:10.1016/j.nuclphysb.2014.10.026http://cds.cern.ch/record/1950179engHentschinski, MartinMartínez, José Daniel MadrigalMurdaca, BeatriceSabio Vera, AgustínThe Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading OrderParticle Physics - PhenomenologyWe complete the computation of the Mueller-Tang jet impact factor at next-to-leading order (NLO) initiated in arXiv:1406.5625 and presented in arXiv:1404.2937 by computing the real corrections associated to gluons in the initial state making use of Lipatov's effective action. NLO corrections for this effective vertex are an important ingredient for a reliable description of large rapidity gap phenomenology within the BFKL approach.We complete the computation of the Mueller–Tang jet impact factor at next-to-leading order (NLO) initiated in [1] and presented in [2] by computing the real corrections associated with gluons in the initial state making use of Lipatov's effective action. NLO corrections for this effective vertex are an important ingredient for a reliable description of large rapidity gap phenomenology within the BFKL approach.We complete the computation of the Mueller-Tang jet impact factor at next-to-leading order (NLO) initiated in arXiv:1406.5625 and presented in arXiv:1404.2937 by computing the real corrections associated to gluons in the initial state making use of Lipatov's effective action. NLO corrections for this effective vertex are an important ingredient for a reliable description of large rapidity gap phenomenology within the BFKL approach.arXiv:1409.6704oai:cds.cern.ch:19501792014-09-23
spellingShingle Particle Physics - Phenomenology
Hentschinski, Martin
Martínez, José Daniel Madrigal
Murdaca, Beatrice
Sabio Vera, Agustín
The Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order
title The Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order
title_full The Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order
title_fullStr The Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order
title_full_unstemmed The Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order
title_short The Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order
title_sort gluon-induced mueller-tang jet impact factor at next-to-leading order
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.nuclphysb.2014.10.026
http://cds.cern.ch/record/1950179
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