All-loop-orders relation between Regge limits of N $$ \mathcal{N} $$ = 4 SYM and N $$ \mathcal{N} $$ = 8 supergravity four-point amplitudes

Abstract We examine in detail the structure of the Regge limit of the (nonplanar) N $$ \mathcal{N} $$ = 4 SYM four-point amplitude. We begin by developing a basis of color factors C ik suitable for the Regge limit of the amplitude at any loop order, and then calculate explicitly the coefficients of...

Full description

Bibliographic Details
Main Author: Stephen G. Naculich
Format: Article
Language:English
Published: SpringerOpen 2021-02-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP02(2021)044
id doaj-39fcb3d7014d4574a448d7cffe2e25b0
record_format Article
spelling doaj-39fcb3d7014d4574a448d7cffe2e25b02021-02-07T12:07:34ZengSpringerOpenJournal of High Energy Physics1029-84792021-02-012021213210.1007/JHEP02(2021)044All-loop-orders relation between Regge limits of N $$ \mathcal{N} $$ = 4 SYM and N $$ \mathcal{N} $$ = 8 supergravity four-point amplitudesStephen G. Naculich0Department of Physics, Bowdoin CollegeAbstract We examine in detail the structure of the Regge limit of the (nonplanar) N $$ \mathcal{N} $$ = 4 SYM four-point amplitude. We begin by developing a basis of color factors C ik suitable for the Regge limit of the amplitude at any loop order, and then calculate explicitly the coefficients of the amplitude in that basis through three-loop order using the Regge limit of the full amplitude previously calculated by Henn and Mistlberger. We compute these coefficients exactly at one loop, through O ϵ 2 $$ \mathcal{O}\left({\upepsilon}^2\right) $$ at two loops, and through O ϵ 0 $$ \mathcal{O}\left({\upepsilon}^0\right) $$ at three loops, verifying that the IR-divergent pieces are consistent with (the Regge limit of) the expected infrared divergence structure, including a contribution from the three-loop correction to the dipole formula. We also verify consistency with the IR-finite NLL and NNLL predictions of Caron-Huot et al. Finally we use these results to motivate the conjecture of an all-orders relation between one of the coefficients and the Regge limit of the N $$ \mathcal{N} $$ = 8 supergravity four-point amplitude.https://doi.org/10.1007/JHEP02(2021)044Extended SupersymmetryScattering AmplitudesSupergravity ModelsSupersymmetric Gauge Theory
collection DOAJ
language English
format Article
sources DOAJ
author Stephen G. Naculich
spellingShingle Stephen G. Naculich
All-loop-orders relation between Regge limits of N $$ \mathcal{N} $$ = 4 SYM and N $$ \mathcal{N} $$ = 8 supergravity four-point amplitudes
Journal of High Energy Physics
Extended Supersymmetry
Scattering Amplitudes
Supergravity Models
Supersymmetric Gauge Theory
author_facet Stephen G. Naculich
author_sort Stephen G. Naculich
title All-loop-orders relation between Regge limits of N $$ \mathcal{N} $$ = 4 SYM and N $$ \mathcal{N} $$ = 8 supergravity four-point amplitudes
title_short All-loop-orders relation between Regge limits of N $$ \mathcal{N} $$ = 4 SYM and N $$ \mathcal{N} $$ = 8 supergravity four-point amplitudes
title_full All-loop-orders relation between Regge limits of N $$ \mathcal{N} $$ = 4 SYM and N $$ \mathcal{N} $$ = 8 supergravity four-point amplitudes
title_fullStr All-loop-orders relation between Regge limits of N $$ \mathcal{N} $$ = 4 SYM and N $$ \mathcal{N} $$ = 8 supergravity four-point amplitudes
title_full_unstemmed All-loop-orders relation between Regge limits of N $$ \mathcal{N} $$ = 4 SYM and N $$ \mathcal{N} $$ = 8 supergravity four-point amplitudes
title_sort all-loop-orders relation between regge limits of n $$ \mathcal{n} $$ = 4 sym and n $$ \mathcal{n} $$ = 8 supergravity four-point amplitudes
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-02-01
description Abstract We examine in detail the structure of the Regge limit of the (nonplanar) N $$ \mathcal{N} $$ = 4 SYM four-point amplitude. We begin by developing a basis of color factors C ik suitable for the Regge limit of the amplitude at any loop order, and then calculate explicitly the coefficients of the amplitude in that basis through three-loop order using the Regge limit of the full amplitude previously calculated by Henn and Mistlberger. We compute these coefficients exactly at one loop, through O ϵ 2 $$ \mathcal{O}\left({\upepsilon}^2\right) $$ at two loops, and through O ϵ 0 $$ \mathcal{O}\left({\upepsilon}^0\right) $$ at three loops, verifying that the IR-divergent pieces are consistent with (the Regge limit of) the expected infrared divergence structure, including a contribution from the three-loop correction to the dipole formula. We also verify consistency with the IR-finite NLL and NNLL predictions of Caron-Huot et al. Finally we use these results to motivate the conjecture of an all-orders relation between one of the coefficients and the Regge limit of the N $$ \mathcal{N} $$ = 8 supergravity four-point amplitude.
topic Extended Supersymmetry
Scattering Amplitudes
Supergravity Models
Supersymmetric Gauge Theory
url https://doi.org/10.1007/JHEP02(2021)044
work_keys_str_mv AT stephengnaculich allloopordersrelationbetweenreggelimitsofnmathcaln4symandnmathcaln8supergravityfourpointamplitudes
_version_ 1724281662052761600