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Beam functions for $N$-jettiness at N$^3$LO in perturbative QCD
We present a calculation of all matching coefficients for N-jettiness beam functions at next-to-next-to-next-to-leading order (N$^{3}$LO) in perturbative quantum chromodynamics (QCD). Our computation is performed starting from the respective collinear splitting kernels, which we integrate using the...
Autores principales: | , , , , |
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Lenguaje: | eng |
Publicado: |
2022
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP02(2023)073 http://cds.cern.ch/record/2840847 |
_version_ | 1780976150060728320 |
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author | Baranowski, Daniel Behring, Arnd Melnikov, Kirill Tancredi, Lorenzo Wever, Christopher |
author_facet | Baranowski, Daniel Behring, Arnd Melnikov, Kirill Tancredi, Lorenzo Wever, Christopher |
author_sort | Baranowski, Daniel |
collection | CERN |
description | We present a calculation of all matching coefficients for N-jettiness beam functions at next-to-next-to-next-to-leading order (N$^{3}$LO) in perturbative quantum chromodynamics (QCD). Our computation is performed starting from the respective collinear splitting kernels, which we integrate using the axial gauge. We use reverse unitarity to map the relevant phase-space integrals to loop integrals, which allows us to employ multi-loop techniques including integration-by-parts identities and differential equations. We find a canonical basis and use an algorithm to establish non-trivial partial fraction relations among the resulting master integrals, which allows us to reduce their number substantially. By use of regularity conditions, we express all necessary boundary constants in terms of an independent set, which we compute by direct integration of the corresponding integrals in the soft limit. In this way, we provide an entirely independent calculation of the matching coefficients which were previously computed in ref. [1]. |
id | cern-2840847 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2022 |
record_format | invenio |
spelling | cern-28408472023-03-04T03:38:03Zdoi:10.1007/JHEP02(2023)073http://cds.cern.ch/record/2840847engBaranowski, DanielBehring, ArndMelnikov, KirillTancredi, LorenzoWever, ChristopherBeam functions for $N$-jettiness at N$^3$LO in perturbative QCDhep-phParticle Physics - PhenomenologyWe present a calculation of all matching coefficients for N-jettiness beam functions at next-to-next-to-next-to-leading order (N$^{3}$LO) in perturbative quantum chromodynamics (QCD). Our computation is performed starting from the respective collinear splitting kernels, which we integrate using the axial gauge. We use reverse unitarity to map the relevant phase-space integrals to loop integrals, which allows us to employ multi-loop techniques including integration-by-parts identities and differential equations. We find a canonical basis and use an algorithm to establish non-trivial partial fraction relations among the resulting master integrals, which allows us to reduce their number substantially. By use of regularity conditions, we express all necessary boundary constants in terms of an independent set, which we compute by direct integration of the corresponding integrals in the soft limit. In this way, we provide an entirely independent calculation of the matching coefficients which were previously computed in ref. [1].We present a calculation of all matching coefficients for $N$-jettiness beam functions at next-to-next-to-next-to-leading order (N$^3$LO) in perturbative quantum chromodynamics (QCD). Our computation is performed starting from the respective collinear splitting kernels, which we integrate using the axial gauge. We use reverse unitarity to map the relevant phase-space integrals to loop integrals, which allows us to employ multi-loop techniques including integration-by-parts identities and differential equations. We find a canonical basis and use an algorithm to establish non-trivial partial fraction relations among the resulting master integrals, which allows us to reduce their number substantially. By use of regularity conditions, we express all necessary boundary constants in terms of an independent set, which we compute by direct integration of the corresponding integrals in the soft limit. In this way, we provide an entirely independent calculation of the matching coefficients which were previously computed in arXiv:2006.03056.arXiv:2211.05722TTP22-067P3H-22-108TUM-HEP-1429/22CERN-TH-2022-178ZU-TH 51/22oai:cds.cern.ch:28408472022-11-10 |
spellingShingle | hep-ph Particle Physics - Phenomenology Baranowski, Daniel Behring, Arnd Melnikov, Kirill Tancredi, Lorenzo Wever, Christopher Beam functions for $N$-jettiness at N$^3$LO in perturbative QCD |
title | Beam functions for $N$-jettiness at N$^3$LO in perturbative QCD |
title_full | Beam functions for $N$-jettiness at N$^3$LO in perturbative QCD |
title_fullStr | Beam functions for $N$-jettiness at N$^3$LO in perturbative QCD |
title_full_unstemmed | Beam functions for $N$-jettiness at N$^3$LO in perturbative QCD |
title_short | Beam functions for $N$-jettiness at N$^3$LO in perturbative QCD |
title_sort | beam functions for $n$-jettiness at n$^3$lo in perturbative qcd |
topic | hep-ph Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/JHEP02(2023)073 http://cds.cern.ch/record/2840847 |
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