Bootstrapping pentagon functions

Abstract In Phys. Rev. Lett. 116 (2016) 062001, the space of planar pentagon functions that describes all two-loop on-shell five-particle scattering amplitudes was introduced. In the present paper we present a natural extension of this space to non-planar pentagon functions. This provides the basis...

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Main Authors: Dmitry Chicherin, Johannes Henn, Vladimir Mitev
Format: Article
Language:English
Published: SpringerOpen 2018-05-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP05(2018)164
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author Dmitry Chicherin
Johannes Henn
Vladimir Mitev
author_facet Dmitry Chicherin
Johannes Henn
Vladimir Mitev
author_sort Dmitry Chicherin
collection DOAJ
description Abstract In Phys. Rev. Lett. 116 (2016) 062001, the space of planar pentagon functions that describes all two-loop on-shell five-particle scattering amplitudes was introduced. In the present paper we present a natural extension of this space to non-planar pentagon functions. This provides the basis for our pentagon bootstrap program. We classify the relevant functions up to weight four, which is relevant for two-loop scattering amplitudes. We constrain the first entry of the symbol of the functions using information on branch cuts. Drawing on an analogy from the planar case, we introduce a conjectural second-entry condition on the symbol. We then show that the information on the function space, when complemented with some additional insights, can be used to efficiently bootstrap individual Feynman integrals. The extra information is read off of Mellin-Barnes representations of the integrals, either by evaluating simple asymptotic limits, or by taking discontinuities in the kinematic variables. We use this method to evaluate the symbols of two non-trivial non-planar five-particle integrals, up to and including the finite part.
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spelling doaj.art-0866c2ab1f574732b9af5d30ae444cd62022-12-21T17:51:09ZengSpringerOpenJournal of High Energy Physics1029-84792018-05-012018512710.1007/JHEP05(2018)164Bootstrapping pentagon functionsDmitry Chicherin0Johannes Henn1Vladimir Mitev2PRISMA Cluster of Excellence, Johannes Gutenberg UniversityPRISMA Cluster of Excellence, Johannes Gutenberg UniversityPRISMA Cluster of Excellence, Johannes Gutenberg UniversityAbstract In Phys. Rev. Lett. 116 (2016) 062001, the space of planar pentagon functions that describes all two-loop on-shell five-particle scattering amplitudes was introduced. In the present paper we present a natural extension of this space to non-planar pentagon functions. This provides the basis for our pentagon bootstrap program. We classify the relevant functions up to weight four, which is relevant for two-loop scattering amplitudes. We constrain the first entry of the symbol of the functions using information on branch cuts. Drawing on an analogy from the planar case, we introduce a conjectural second-entry condition on the symbol. We then show that the information on the function space, when complemented with some additional insights, can be used to efficiently bootstrap individual Feynman integrals. The extra information is read off of Mellin-Barnes representations of the integrals, either by evaluating simple asymptotic limits, or by taking discontinuities in the kinematic variables. We use this method to evaluate the symbols of two non-trivial non-planar five-particle integrals, up to and including the finite part.http://link.springer.com/article/10.1007/JHEP05(2018)164Scattering AmplitudesPerturbative QCD
spellingShingle Dmitry Chicherin
Johannes Henn
Vladimir Mitev
Bootstrapping pentagon functions
Journal of High Energy Physics
Scattering Amplitudes
Perturbative QCD
title Bootstrapping pentagon functions
title_full Bootstrapping pentagon functions
title_fullStr Bootstrapping pentagon functions
title_full_unstemmed Bootstrapping pentagon functions
title_short Bootstrapping pentagon functions
title_sort bootstrapping pentagon functions
topic Scattering Amplitudes
Perturbative QCD
url http://link.springer.com/article/10.1007/JHEP05(2018)164
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