The structure of IR divergences in celestial gluon amplitudes

Abstract The all-loop resummation of SU(N) gauge theory amplitudes is known to factorize into an IR-divergent (soft and collinear) factor and a finite (hard) piece. The divergent factor is universal, whereas the hard function is a process-dependent quantity. We prove that this factorization persists...

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Main Authors: Hernán A. González, Francisco Rojas
Format: Article
Language:English
Published: SpringerOpen 2021-06-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP06(2021)171
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spelling doaj-db9b973422f44ec597be21e6eea9c80b2021-07-04T11:52:11ZengSpringerOpenJournal of High Energy Physics1029-84792021-06-012021612710.1007/JHEP06(2021)171The structure of IR divergences in celestial gluon amplitudesHernán A. González0Francisco Rojas1Departamento de Ciencias, Facultad de Artes Liberales, Universidad Adolfo IbáñezFacultad de Ingeniería y Ciencias, Universidad Adolfo IbáñezAbstract The all-loop resummation of SU(N) gauge theory amplitudes is known to factorize into an IR-divergent (soft and collinear) factor and a finite (hard) piece. The divergent factor is universal, whereas the hard function is a process-dependent quantity. We prove that this factorization persists for the corresponding celestial amplitudes. Moreover, the soft/collinear factor becomes a scalar correlator of the product of renormalized Wilson lines defined in terms of celestial data. Their effect on the hard amplitude is a shift in the scaling dimensions by an infinite amount, proportional to the cusp anomalous dimension. This leads us to conclude that the celestial-IR-safe gluon amplitude corresponds to a expectation value of operators dressed with Wilson line primaries. These results hold for finite N. In the large N limit, we show that the soft/collinear correlator can be described in terms of vertex operators in a Coulomb gas of colored scalar primaries with nearest neighbor interactions. In the particular cases of four and five gluons in planar N $$ \mathcal{N} $$ = 4 SYM theory, where the hard factor is known to exponentiate, we establish that the Mellin transform converges in the UV thanks to the fact that the cusp anomalous dimension is a positive quantity. In other words, the very existence of the full celestial amplitude is owed to the positivity of the cusp anomalous dimension.https://doi.org/10.1007/JHEP06(2021)171Conformal Field TheoryScattering AmplitudesField Theories in Lower Dimensions
collection DOAJ
language English
format Article
sources DOAJ
author Hernán A. González
Francisco Rojas
spellingShingle Hernán A. González
Francisco Rojas
The structure of IR divergences in celestial gluon amplitudes
Journal of High Energy Physics
Conformal Field Theory
Scattering Amplitudes
Field Theories in Lower Dimensions
author_facet Hernán A. González
Francisco Rojas
author_sort Hernán A. González
title The structure of IR divergences in celestial gluon amplitudes
title_short The structure of IR divergences in celestial gluon amplitudes
title_full The structure of IR divergences in celestial gluon amplitudes
title_fullStr The structure of IR divergences in celestial gluon amplitudes
title_full_unstemmed The structure of IR divergences in celestial gluon amplitudes
title_sort structure of ir divergences in celestial gluon amplitudes
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-06-01
description Abstract The all-loop resummation of SU(N) gauge theory amplitudes is known to factorize into an IR-divergent (soft and collinear) factor and a finite (hard) piece. The divergent factor is universal, whereas the hard function is a process-dependent quantity. We prove that this factorization persists for the corresponding celestial amplitudes. Moreover, the soft/collinear factor becomes a scalar correlator of the product of renormalized Wilson lines defined in terms of celestial data. Their effect on the hard amplitude is a shift in the scaling dimensions by an infinite amount, proportional to the cusp anomalous dimension. This leads us to conclude that the celestial-IR-safe gluon amplitude corresponds to a expectation value of operators dressed with Wilson line primaries. These results hold for finite N. In the large N limit, we show that the soft/collinear correlator can be described in terms of vertex operators in a Coulomb gas of colored scalar primaries with nearest neighbor interactions. In the particular cases of four and five gluons in planar N $$ \mathcal{N} $$ = 4 SYM theory, where the hard factor is known to exponentiate, we establish that the Mellin transform converges in the UV thanks to the fact that the cusp anomalous dimension is a positive quantity. In other words, the very existence of the full celestial amplitude is owed to the positivity of the cusp anomalous dimension.
topic Conformal Field Theory
Scattering Amplitudes
Field Theories in Lower Dimensions
url https://doi.org/10.1007/JHEP06(2021)171
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