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The quark induced Mueller-Tang jet impact factor at next-to-leading order

We present the NLO corrections for the quark induced forward production of a jet with an associated rapidity gap. We make use of Lipatov's QCD high energy effective action to calculate the real emission contributions to the so-called Mueller-Tang impact factor. We combine them with the previous...

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Detalles Bibliográficos
Autores principales: Hentschinski, M., Madrigal Martínez, J.D., Murdaca, B., Sabio Vera, A.
Lenguaje:eng
Publicado: 2014
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2014.08.010
http://cds.cern.ch/record/1711495
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author Hentschinski, M.
Madrigal Martínez, J.D.
Murdaca, B.
Sabio Vera, A.
author_facet Hentschinski, M.
Madrigal Martínez, J.D.
Murdaca, B.
Sabio Vera, A.
author_sort Hentschinski, M.
collection CERN
description We present the NLO corrections for the quark induced forward production of a jet with an associated rapidity gap. We make use of Lipatov's QCD high energy effective action to calculate the real emission contributions to the so-called Mueller-Tang impact factor. We combine them with the previously calculated virtual corrections and verify ultraviolet and collinear finiteness of the final result.
id cern-1711495
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2014
record_format invenio
spelling cern-17114952023-10-04T08:17:56Zdoi:10.1016/j.nuclphysb.2014.08.010http://cds.cern.ch/record/1711495engHentschinski, M.Madrigal Martínez, J.D.Murdaca, B.Sabio Vera, A.The quark induced Mueller-Tang jet impact factor at next-to-leading orderhep-phWe present the NLO corrections for the quark induced forward production of a jet with an associated rapidity gap. We make use of Lipatov's QCD high energy effective action to calculate the real emission contributions to the so-called Mueller-Tang impact factor. We combine them with the previously calculated virtual corrections and verify ultraviolet and collinear finiteness of the final result.We present the NLO corrections for the quark induced forward production of a jet with an associated rapidity gap. We make use of Lipatov's QCD high energy effective action to calculate the real emission contributions to the so-called Mueller–Tang impact factor. We combine them with the previously calculated virtual corrections and verify ultraviolet and collinear finiteness of the final result.We present the NLO corrections for the quark induced forward production of a jet with an associated rapidity gap. We make use of Lipatov's QCD high energy effective action to calculate the real emission contributions to the so-called Mueller-Tang impact factor. We combine them with the previously calculated virtual corrections and verify ultraviolet and collinear finiteness of the final result.arXiv:1406.5625CERN-PH-TH-2014-115CERN-PH-TH-2014-115oai:cds.cern.ch:17114952014-06-21
spellingShingle hep-ph
Hentschinski, M.
Madrigal Martínez, J.D.
Murdaca, B.
Sabio Vera, A.
The quark induced Mueller-Tang jet impact factor at next-to-leading order
title The quark induced Mueller-Tang jet impact factor at next-to-leading order
title_full The quark induced Mueller-Tang jet impact factor at next-to-leading order
title_fullStr The quark induced Mueller-Tang jet impact factor at next-to-leading order
title_full_unstemmed The quark induced Mueller-Tang jet impact factor at next-to-leading order
title_short The quark induced Mueller-Tang jet impact factor at next-to-leading order
title_sort quark induced mueller-tang jet impact factor at next-to-leading order
topic hep-ph
url https://dx.doi.org/10.1016/j.nuclphysb.2014.08.010
http://cds.cern.ch/record/1711495
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