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The seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracy

We present an all-loop dispersion integral, well-defined to arbitrary logarithmic accuracy, describing the multi-Regge limit of the 2 → 5 amplitude in planar $ \mathcal{N}=4 $ super Yang-Mills theory. It follows from factorization, dual conformal symmetry and consistency with soft limits, and specif...

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Autores principales: Del Duca, Vittorio, Druc, Stefan, Drummond, James, Duhr, Claude, Dulat, Falko, Marzucca, Robin, Papathanasiou, Georgios, Verbeek, Bram
Lenguaje:eng
Publicado: 2018
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP06(2018)116
http://cds.cern.ch/record/2307388
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author Del Duca, Vittorio
Druc, Stefan
Drummond, James
Duhr, Claude
Dulat, Falko
Marzucca, Robin
Papathanasiou, Georgios
Verbeek, Bram
author_facet Del Duca, Vittorio
Druc, Stefan
Drummond, James
Duhr, Claude
Dulat, Falko
Marzucca, Robin
Papathanasiou, Georgios
Verbeek, Bram
author_sort Del Duca, Vittorio
collection CERN
description We present an all-loop dispersion integral, well-defined to arbitrary logarithmic accuracy, describing the multi-Regge limit of the 2 → 5 amplitude in planar $ \mathcal{N}=4 $ super Yang-Mills theory. It follows from factorization, dual conformal symmetry and consistency with soft limits, and specifically holds in the region where the energies of all produced particles have been analytically continued. After promoting the known symbol of the 2-loop N -particle MHV amplitude in this region to a function, we specialize to N = 7, and extract from it the next-to-leading order (NLO) correction to the BFKL central emission vertex, namely the building block of the dispersion integral that had not yet appeared in the well-studied six-gluon case. As an application of our results, we explicitly compute the seven-gluon amplitude at next-to-leading logarithmic accuracy through 5 loops for the MHV case, and through 3 and 4 loops for the two independent NMHV helicity configurations, respectively.
id cern-2307388
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2018
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spelling cern-23073882023-10-04T06:07:50Zdoi:10.1007/JHEP06(2018)116http://cds.cern.ch/record/2307388engDel Duca, VittorioDruc, StefanDrummond, JamesDuhr, ClaudeDulat, FalkoMarzucca, RobinPapathanasiou, GeorgiosVerbeek, BramThe seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracyhep-thParticle Physics - TheoryWe present an all-loop dispersion integral, well-defined to arbitrary logarithmic accuracy, describing the multi-Regge limit of the 2 → 5 amplitude in planar $ \mathcal{N}=4 $ super Yang-Mills theory. It follows from factorization, dual conformal symmetry and consistency with soft limits, and specifically holds in the region where the energies of all produced particles have been analytically continued. After promoting the known symbol of the 2-loop N -particle MHV amplitude in this region to a function, we specialize to N = 7, and extract from it the next-to-leading order (NLO) correction to the BFKL central emission vertex, namely the building block of the dispersion integral that had not yet appeared in the well-studied six-gluon case. As an application of our results, we explicitly compute the seven-gluon amplitude at next-to-leading logarithmic accuracy through 5 loops for the MHV case, and through 3 and 4 loops for the two independent NMHV helicity configurations, respectively.We present an all-loop dispersion integral, well-defined to arbitrary logarithmic accuracy, describing the multi-Regge limit of the 2->5 amplitude in planar N=4 super Yang-Mills theory. It follows from factorization, dual conformal symmetry and consistency with soft limits, and specifically holds in the region where the energies of all produced particles have been analytically continued. After promoting the known symbol of the 2-loop N-particle MHV amplitude in this region to a function, we specialize to N=7, and extract from it the next-to-leading order (NLO) correction to the BFKL central emission vertex, namely the building block of the dispersion integral that had not yet appeared in the well-studied six-gluon case. As an application of our results, we explicitly compute the seven-gluon amplitude at next-to-leading logarithmic accuracy through 5 loops for the MHV case, and through 3 and 4 loops for the two independent NMHV helicity configurations, respectively.arXiv:1801.10605DESY-18-009CERN-TH-2018-016CP3-18-06SLAC-PUB-17220oai:cds.cern.ch:23073882018-01-31
spellingShingle hep-th
Particle Physics - Theory
Del Duca, Vittorio
Druc, Stefan
Drummond, James
Duhr, Claude
Dulat, Falko
Marzucca, Robin
Papathanasiou, Georgios
Verbeek, Bram
The seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracy
title The seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracy
title_full The seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracy
title_fullStr The seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracy
title_full_unstemmed The seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracy
title_short The seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracy
title_sort seven-gluon amplitude in multi-regge kinematics beyond leading logarithmic accuracy
topic hep-th
Particle Physics - Theory
url https://dx.doi.org/10.1007/JHEP06(2018)116
http://cds.cern.ch/record/2307388
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