The S matrix of 6D super Yang-Mills and maximal supergravity from rational maps

Abstract We present new formulas for n-particle tree-level scattering amplitudes of six-dimensional N=11 $$ \mathcal{N}=\left(1,1\right) $$ super Yang-Mills (SYM) and N=22 $$ \mathcal{N}=\left(2,2\right) $$ supergravity (SUGRA). They are written as integrals over the moduli space of certain rational...

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Main Authors: Freddy Cachazo, Alfredo Guevara, Matthew Heydeman, Sebastian Mizera, John H. Schwarz, Congkao Wen
Format: Article
Language:English
Published: SpringerOpen 2018-09-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP09(2018)125
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author Freddy Cachazo
Alfredo Guevara
Matthew Heydeman
Sebastian Mizera
John H. Schwarz
Congkao Wen
author_facet Freddy Cachazo
Alfredo Guevara
Matthew Heydeman
Sebastian Mizera
John H. Schwarz
Congkao Wen
author_sort Freddy Cachazo
collection DOAJ
description Abstract We present new formulas for n-particle tree-level scattering amplitudes of six-dimensional N=11 $$ \mathcal{N}=\left(1,1\right) $$ super Yang-Mills (SYM) and N=22 $$ \mathcal{N}=\left(2,2\right) $$ supergravity (SUGRA). They are written as integrals over the moduli space of certain rational maps localized on the (n − 3)! solutions of the scattering equations. Due to the properties of spinor-helicity variables in six dimensions, the even-n and odd-n formulas are quite different and have to be treated separately. We first propose a manifestly supersymmetric expression for the even-n amplitudes of N=11 $$ \mathcal{N}=\left(1,1\right) $$ SYM theory and perform various consistency checks. By considering soft-gluon limits of the even-n amplitudes, we deduce the form of the rational maps and the integrand for n odd. The odd-n formulas obtained in this way have a new redundancy that is intertwined with the usual SL(2, ℂ) invariance on the Riemann sphere. We also propose an alternative form of the formulas, analogous to the Witten-RSV formulation, and explore its relationship with the symplectic (or Lagrangian) Grassmannian. Since the amplitudes are formulated in a way that manifests double-copy properties, formulas for the six-dimensional N=22 $$ \mathcal{N}=\left(2,2\right) $$ SUGRA amplitudes follow. These six-dimensional results allow us to deduce new formulas for five-dimensional SYM and SUGRA amplitudes, as well as massive amplitudes of four-dimensional N=4 $$ \mathcal{N}=4 $$ SYM on the Coulomb branch.
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spelling doaj.art-5b4cd6eb2ea84d468f478f6ab1e215282022-12-21T19:49:10ZengSpringerOpenJournal of High Energy Physics1029-84792018-09-012018918610.1007/JHEP09(2018)125The S matrix of 6D super Yang-Mills and maximal supergravity from rational mapsFreddy Cachazo0Alfredo Guevara1Matthew Heydeman2Sebastian Mizera3John H. Schwarz4Congkao Wen5Perimeter Institute for Theoretical PhysicsPerimeter Institute for Theoretical PhysicsWalter Burke Institute for Theoretical Physics, California Institute of Technology 452-48Perimeter Institute for Theoretical PhysicsWalter Burke Institute for Theoretical Physics, California Institute of Technology 452-48Walter Burke Institute for Theoretical Physics, California Institute of Technology 452-48Abstract We present new formulas for n-particle tree-level scattering amplitudes of six-dimensional N=11 $$ \mathcal{N}=\left(1,1\right) $$ super Yang-Mills (SYM) and N=22 $$ \mathcal{N}=\left(2,2\right) $$ supergravity (SUGRA). They are written as integrals over the moduli space of certain rational maps localized on the (n − 3)! solutions of the scattering equations. Due to the properties of spinor-helicity variables in six dimensions, the even-n and odd-n formulas are quite different and have to be treated separately. We first propose a manifestly supersymmetric expression for the even-n amplitudes of N=11 $$ \mathcal{N}=\left(1,1\right) $$ SYM theory and perform various consistency checks. By considering soft-gluon limits of the even-n amplitudes, we deduce the form of the rational maps and the integrand for n odd. The odd-n formulas obtained in this way have a new redundancy that is intertwined with the usual SL(2, ℂ) invariance on the Riemann sphere. We also propose an alternative form of the formulas, analogous to the Witten-RSV formulation, and explore its relationship with the symplectic (or Lagrangian) Grassmannian. Since the amplitudes are formulated in a way that manifests double-copy properties, formulas for the six-dimensional N=22 $$ \mathcal{N}=\left(2,2\right) $$ SUGRA amplitudes follow. These six-dimensional results allow us to deduce new formulas for five-dimensional SYM and SUGRA amplitudes, as well as massive amplitudes of four-dimensional N=4 $$ \mathcal{N}=4 $$ SYM on the Coulomb branch.http://link.springer.com/article/10.1007/JHEP09(2018)125Scattering AmplitudesField Theories in Higher DimensionsSupersymmetric Gauge Theory
spellingShingle Freddy Cachazo
Alfredo Guevara
Matthew Heydeman
Sebastian Mizera
John H. Schwarz
Congkao Wen
The S matrix of 6D super Yang-Mills and maximal supergravity from rational maps
Journal of High Energy Physics
Scattering Amplitudes
Field Theories in Higher Dimensions
Supersymmetric Gauge Theory
title The S matrix of 6D super Yang-Mills and maximal supergravity from rational maps
title_full The S matrix of 6D super Yang-Mills and maximal supergravity from rational maps
title_fullStr The S matrix of 6D super Yang-Mills and maximal supergravity from rational maps
title_full_unstemmed The S matrix of 6D super Yang-Mills and maximal supergravity from rational maps
title_short The S matrix of 6D super Yang-Mills and maximal supergravity from rational maps
title_sort s matrix of 6d super yang mills and maximal supergravity from rational maps
topic Scattering Amplitudes
Field Theories in Higher Dimensions
Supersymmetric Gauge Theory
url http://link.springer.com/article/10.1007/JHEP09(2018)125
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