Four-graviton scattering to three loops in N = 8 $$ \mathcal{N}=8 $$ supergravity

Abstract We compute the three-loop scattering amplitude of four gravitons in N = 8...

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Main Authors: Henn, J. M, Mistlberger, B.
Other Authors: Massachusetts Institute of Technology. Center for Theoretical Physics
Format: Article
Language:English
Published: Springer Berlin Heidelberg 2021
Online Access:https://hdl.handle.net/1721.1/131680
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author Henn, J. M
Mistlberger, B.
author2 Massachusetts Institute of Technology. Center for Theoretical Physics
author_facet Massachusetts Institute of Technology. Center for Theoretical Physics
Henn, J. M
Mistlberger, B.
author_sort Henn, J. M
collection MIT
description Abstract We compute the three-loop scattering amplitude of four gravitons in N = 8 $$ \mathcal{N}=8 $$ supergravity. Our results are analytic formulae for a Laurent expansion of the amplitude in the regulator of dimensional regularisation. The coefficients of this series are closed formulae in terms of well-established harmonic poly-logarithms. Our results display a remarkable degree of simplicity and represent an important stepping stone in the exploration of the structure of scattering amplitudes. In particular, we observe that to this loop order the four graviton amplitude is given by uniform weight 2L functions, where L is the loop order.
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spelling mit-1721.1/1316802023-02-23T20:54:54Z Four-graviton scattering to three loops in N = 8 $$ \mathcal{N}=8 $$ supergravity Henn, J. M Mistlberger, B. Massachusetts Institute of Technology. Center for Theoretical Physics Abstract We compute the three-loop scattering amplitude of four gravitons in N = 8 $$ \mathcal{N}=8 $$ supergravity. Our results are analytic formulae for a Laurent expansion of the amplitude in the regulator of dimensional regularisation. The coefficients of this series are closed formulae in terms of well-established harmonic poly-logarithms. Our results display a remarkable degree of simplicity and represent an important stepping stone in the exploration of the structure of scattering amplitudes. In particular, we observe that to this loop order the four graviton amplitude is given by uniform weight 2L functions, where L is the loop order. 2021-09-20T17:29:35Z 2021-09-20T17:29:35Z 2019-05-03 2020-06-26T12:59:59Z Article http://purl.org/eprint/type/JournalArticle https://hdl.handle.net/1721.1/131680 Journal of High Energy Physics. 2019 May 03;2019(5):23 PUBLISHER_CC en https://doi.org/10.1007/JHEP05(2019)023 Creative Commons Attribution https://creativecommons.org/licenses/by/4.0/ The Author(s) application/pdf Springer Berlin Heidelberg Springer Berlin Heidelberg
spellingShingle Henn, J. M
Mistlberger, B.
Four-graviton scattering to three loops in N = 8 $$ \mathcal{N}=8 $$ supergravity
title Four-graviton scattering to three loops in N = 8 $$ \mathcal{N}=8 $$ supergravity
title_full Four-graviton scattering to three loops in N = 8 $$ \mathcal{N}=8 $$ supergravity
title_fullStr Four-graviton scattering to three loops in N = 8 $$ \mathcal{N}=8 $$ supergravity
title_full_unstemmed Four-graviton scattering to three loops in N = 8 $$ \mathcal{N}=8 $$ supergravity
title_short Four-graviton scattering to three loops in N = 8 $$ \mathcal{N}=8 $$ supergravity
title_sort four graviton scattering to three loops in n 8 mathcal n 8 supergravity
url https://hdl.handle.net/1721.1/131680
work_keys_str_mv AT hennjm fourgravitonscatteringtothreeloopsinn8mathcaln8supergravity
AT mistlbergerb fourgravitonscatteringtothreeloopsinn8mathcaln8supergravity