All one-loop NMHV gluon amplitudes in $ \mathcal{N} $ = 1 SYM

We compute the next-to-maximally-helicity-violating one-loop n-gluon amplitudes in N = 1 super-Yang-Mills theory. These amplitudes contain three negative-helicity gluons and an arbitrary number of positive-helicity gluons, and constitute the first infinite series of amplitudes beyond the simplest, M...

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Autor principal: Ochirov, A
Formato: Journal article
Idioma:English
Publicado em: Springer 2013
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author Ochirov, A
author_facet Ochirov, A
author_sort Ochirov, A
collection OXFORD
description We compute the next-to-maximally-helicity-violating one-loop n-gluon amplitudes in N = 1 super-Yang-Mills theory. These amplitudes contain three negative-helicity gluons and an arbitrary number of positive-helicity gluons, and constitute the first infinite series of amplitudes beyond the simplest, MHV, amplitudes. We assemble ingredients from the N = 4 NMHV tree super-amplitude into previously unwritten double cuts and use the spinor integration technique to calculate all bubble coefficients. We also derive the missing box coefficients from quadruple cuts. Together with the known formula for three-mass triangles, this completes the set of NMHV one-loop master integral coefficients in N = 1 SYM. To facilitate further use of our results, we provide their Mathematica implementation.
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spelling oxford-uuid:f1c9dc48-d503-40ea-9cc0-6b3e4cdda2e92022-03-27T11:58:41ZAll one-loop NMHV gluon amplitudes in $ \mathcal{N} $ = 1 SYMJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:f1c9dc48-d503-40ea-9cc0-6b3e4cdda2e9EnglishSymplectic ElementsSpringer2013Ochirov, AWe compute the next-to-maximally-helicity-violating one-loop n-gluon amplitudes in N = 1 super-Yang-Mills theory. These amplitudes contain three negative-helicity gluons and an arbitrary number of positive-helicity gluons, and constitute the first infinite series of amplitudes beyond the simplest, MHV, amplitudes. We assemble ingredients from the N = 4 NMHV tree super-amplitude into previously unwritten double cuts and use the spinor integration technique to calculate all bubble coefficients. We also derive the missing box coefficients from quadruple cuts. Together with the known formula for three-mass triangles, this completes the set of NMHV one-loop master integral coefficients in N = 1 SYM. To facilitate further use of our results, we provide their Mathematica implementation.
spellingShingle Ochirov, A
All one-loop NMHV gluon amplitudes in $ \mathcal{N} $ = 1 SYM
title All one-loop NMHV gluon amplitudes in $ \mathcal{N} $ = 1 SYM
title_full All one-loop NMHV gluon amplitudes in $ \mathcal{N} $ = 1 SYM
title_fullStr All one-loop NMHV gluon amplitudes in $ \mathcal{N} $ = 1 SYM
title_full_unstemmed All one-loop NMHV gluon amplitudes in $ \mathcal{N} $ = 1 SYM
title_short All one-loop NMHV gluon amplitudes in $ \mathcal{N} $ = 1 SYM
title_sort all one loop nmhv gluon amplitudes in mathcal n 1 sym
work_keys_str_mv AT ochirova alloneloopnmhvgluonamplitudesinmathcaln1sym