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High-energy limit of 2->2 scattering amplitudes at NNLL
The high-energy limit of $2\to 2$ scattering amplitudes offers an excellent setting to explore the universal features of gauge theories. At Leading Logarithmic (LL) accuracy the partonic amplitude is governed by Regge poles in the complex angular momentum plane. Beyond LL, Regge cuts in this plane b...
Autores principales: | , , , , |
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Lenguaje: | eng |
Publicado: |
2022
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.22323/1.416.0044 http://cds.cern.ch/record/2861062 |
_version_ | 1780977791260426240 |
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author | Milloy, Calum Falcioni, Giulio Gardi, Einan Maher, Niamh Vernazza, Leonardo |
author_facet | Milloy, Calum Falcioni, Giulio Gardi, Einan Maher, Niamh Vernazza, Leonardo |
author_sort | Milloy, Calum |
collection | CERN |
description | The high-energy limit of $2\to 2$ scattering amplitudes offers an excellent setting to explore the universal features of gauge theories. At Leading Logarithmic (LL) accuracy the partonic amplitude is governed by Regge poles in the complex angular momentum plane. Beyond LL, Regge cuts in this plane begin to play an important role. Specifically, the real part of the amplitude at Next-to-Next-to-Leading Logarithmic (NNLL) accuracy presents for the first time both a Regge pole and a Regge cut. Analysing this tower of logarithms and computing it explicitly through four loops we are able to systematically separate between the Regge pole and the Regge cut. The former involves two fundamental parameters, namely the gluon Regge trajectory and impact factors. We explain how to consistently define the impact factors at two loops and the Regge trajectory at three loops. We confirm that the singularities of the trajectory are given by the cusp anomalous dimension. We also show that the Regge-cut contribution at four loop is nonplanar. |
id | cern-2861062 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2022 |
record_format | invenio |
spelling | cern-28610622023-06-29T04:20:57Zdoi:10.22323/1.416.0044http://cds.cern.ch/record/2861062engMilloy, CalumFalcioni, GiulioGardi, EinanMaher, NiamhVernazza, LeonardoHigh-energy limit of 2->2 scattering amplitudes at NNLLhep-thParticle Physics - Theoryhep-phParticle Physics - PhenomenologyThe high-energy limit of $2\to 2$ scattering amplitudes offers an excellent setting to explore the universal features of gauge theories. At Leading Logarithmic (LL) accuracy the partonic amplitude is governed by Regge poles in the complex angular momentum plane. Beyond LL, Regge cuts in this plane begin to play an important role. Specifically, the real part of the amplitude at Next-to-Next-to-Leading Logarithmic (NNLL) accuracy presents for the first time both a Regge pole and a Regge cut. Analysing this tower of logarithms and computing it explicitly through four loops we are able to systematically separate between the Regge pole and the Regge cut. The former involves two fundamental parameters, namely the gluon Regge trajectory and impact factors. We explain how to consistently define the impact factors at two loops and the Regge trajectory at three loops. We confirm that the singularities of the trajectory are given by the cusp anomalous dimension. We also show that the Regge-cut contribution at four loop is nonplanar.The high-energy limit of $2\to 2$ scattering amplitudes offers an excellent setting to explore the universal features of gauge theories. At Leading Logarithmic (LL) accuracy the partonic amplitude is governed by Regge poles in the complex angular momentum plane. Beyond LL, Regge cuts in this plane begin to play an important role. Specifically, the real part of the amplitude at Next-to-Next-to-Leading Logarithmic (NNLL) accuracy presents for the first time both a Regge pole and a Regge cut. Analysing this tower of logarithms and computing it explicitly through four loops we are able to systematically separate between the Regge pole and the Regge cut. The former involves two fundamental parameters, namely the gluon Regge trajectory and impact factors. We explain how to consistently define the impact factors at two loops and the Regge trajectory at three loops. We confirm that the singularities of the trajectory are given by the cusp anomalous dimension. We also show that the Regge-cut contribution at four loop is nonplanar.arXiv:2207.07441oai:cds.cern.ch:28610622022-07-15 |
spellingShingle | hep-th Particle Physics - Theory hep-ph Particle Physics - Phenomenology Milloy, Calum Falcioni, Giulio Gardi, Einan Maher, Niamh Vernazza, Leonardo High-energy limit of 2->2 scattering amplitudes at NNLL |
title | High-energy limit of 2->2 scattering amplitudes at NNLL |
title_full | High-energy limit of 2->2 scattering amplitudes at NNLL |
title_fullStr | High-energy limit of 2->2 scattering amplitudes at NNLL |
title_full_unstemmed | High-energy limit of 2->2 scattering amplitudes at NNLL |
title_short | High-energy limit of 2->2 scattering amplitudes at NNLL |
title_sort | high-energy limit of 2->2 scattering amplitudes at nnll |
topic | hep-th Particle Physics - Theory hep-ph Particle Physics - Phenomenology |
url | https://dx.doi.org/10.22323/1.416.0044 http://cds.cern.ch/record/2861062 |
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