002307388 001__ 2307388
002307388 005__ 20231130044503.0
002307388 0248_ $$aoai:cds.cern.ch:2307388$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
002307388 0247_ $$2DOI$$9bibmatch$$a10.1007/JHEP06(2018)116
002307388 037__ $$9arXiv$$aarXiv:1801.10605$$chep-th
002307388 037__ $$aDESY-18-009
002307388 037__ $$aCERN-TH-2018-016
002307388 037__ $$aCP3-18-06
002307388 037__ $$aSLAC-PUB-17220
002307388 035__ $$9arXiv$$aoai:arXiv.org:1801.10605
002307388 035__ $$9Inspire$$aoai:inspirehep.net:1651508$$d2023-11-29T09:52:47Z$$h2023-11-30T03:00:02Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002307388 035__ $$9Inspire$$a1651508
002307388 041__ $$aeng
002307388 100__ $$aDel Duca, Vittorio$$uZurich, ETH$$vOn leave from Istituto Nazionale di Fisica Nucleare, Laboratori Nazionali di Frascati, Italy$$vInstitute for Theoretical Physics - ETH Zürich - 8093 - Zürich - Switzerland
002307388 245__ $$9arXiv$$aThe seven-gluon amplitude in multi-Regge kinematics beyond leading logarithmic accuracy
002307388 269__ $$c2018-01-31
002307388 260__ $$c2018-06-21
002307388 300__ $$a56 p
002307388 500__ $$9Inspire$$a* Temporary entry *
002307388 500__ $$9arXiv$$a56 pages, 4 figures, 1 table; v2: minor corrections and
clarifications, matches published version
002307388 520__ $$9Springer$$aWe present an all-loop dispersion integral, well-defined to arbitrary logarithmic accuracy, describing the multi-Regge limit of the 2 → 5 amplitude in planar $ \mathcal{N}=4 $ super Yang-Mills theory. It follows from factorization, dual conformal symmetry and consistency with soft limits, and specifically holds in the region where the energies of all produced particles have been analytically continued. After promoting the known symbol of the 2-loop N -particle MHV amplitude in this region to a function, we specialize to N = 7, and extract from it the next-to-leading order (NLO) correction to the BFKL central emission vertex, namely the building block of the dispersion integral that had not yet appeared in the well-studied six-gluon case. As an application of our results, we explicitly compute the seven-gluon amplitude at next-to-leading logarithmic accuracy through 5 loops for the MHV case, and through 3 and 4 loops for the two independent NMHV helicity configurations, respectively.
002307388 520__ $$9arXiv$$aWe present an all-loop dispersion integral, well-defined to arbitrary logarithmic accuracy, describing the multi-Regge limit of the 2->5 amplitude in planar N=4 super Yang-Mills theory. It follows from factorization, dual conformal symmetry and consistency with soft limits, and specifically holds in the region where the energies of all produced particles have been analytically continued. After promoting the known symbol of the 2-loop N-particle MHV amplitude in this region to a function, we specialize to N=7, and extract from it the next-to-leading order (NLO) correction to the BFKL central emission vertex, namely the building block of the dispersion integral that had not yet appeared in the well-studied six-gluon case. As an application of our results, we explicitly compute the seven-gluon amplitude at next-to-leading logarithmic accuracy through 5 loops for the MHV case, and through 3 and 4 loops for the two independent NMHV helicity configurations, respectively.
002307388 540__ $$3preprint$$aarXiv nonexclusive-distrib 1.0$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002307388 540__ $$3publication$$9Springer$$aCC-BY-4.0
002307388 595__ $$aCERN-TH
002307388 65017 $$2arXiv$$ahep-th
002307388 65017 $$2SzGeCERN$$aParticle Physics - Theory
002307388 690C_ $$aCERN
002307388 690C_ $$aARTICLE
002307388 700__ $$aDruc, Stefan$$tGRID:grid.5491.9$$uSouthampton U.$$vSchool of Physics & Astronomy, University of Southampton, Highfield, SO17 1BJ Southampton, United Kingdom
002307388 700__ $$aDrummond, James$$tGRID:grid.5491.9$$uSouthampton U.$$vSchool of Physics & Astronomy, University of Southampton, Highfield, SO17 1BJ Southampton, United Kingdom
002307388 700__ $$aDuhr, Claude$$tGRID:grid.9132.9$$tGRID:grid.7942.8$$uCERN$$uLouvain U., CP3$$vTheoretical Physics Department, CERN, CH-1211 Geneva 23, Switzerland$$vCenter for Cosmology, Particle Physics and Phenomenology (CP3), Université catholique de Louvain, Chemin du Cyclotron 2, 1348 Louvain-La-Neuve, Belgium
002307388 700__ $$aDulat, Falko$$tGRID:grid.168010.e$$uSLAC$$vSLAC National Accelerator Laboratory, Stanford University, 94309 Stanford, USA
002307388 700__ $$aMarzucca, Robin$$tGRID:grid.7942.8$$uLouvain U., CP3$$vCenter for Cosmology, Particle Physics and Phenomenology (CP3), Université catholique de Louvain, Chemin du Cyclotron 2, 1348 Louvain-La-Neuve, Belgium
002307388 700__ $$aPapathanasiou, Georgios$$iINSPIRE-00349605$$jORCID:0000-0002-2627-9906$$tGRID:grid.7683.a$$uDESY$$vDESY Theory Group, DESY Hamburg, Notkestraße 85, D-22607 Hamburg, Germany
002307388 700__ $$aVerbeek, Bram$$tGRID:grid.7942.8$$uLouvain U., CP3$$vCenter for Cosmology, Particle Physics and Phenomenology (CP3), Université catholique de Louvain, Chemin du Cyclotron 2, 1348 Louvain-La-Neuve, Belgium
002307388 773__ $$c116$$pJHEP$$v06$$y2018
002307388 8564_ $$81388477$$s847621$$uhttps://cds.cern.ch/record/2307388/files/arXiv:1801.10605.pdf
002307388 8564_ $$81414473$$s1077782$$uhttps://cds.cern.ch/record/2307388/files/scoap3-fulltext.pdf$$yArticle from SCOAP3
002307388 8564_ $$82335224$$s1077782$$uhttps://cds.cern.ch/record/2307388/files/scoap.pdf$$yArticle from SCOAP3
002307388 960__ $$a13
002307388 980__ $$aARTICLE