4.4 Article

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

Journal

JOURNAL OF HIGH ENERGY PHYSICS
Volume -, Issue 9, Pages -

Publisher

SPRINGER
DOI: 10.1007/JHEP09(2018)125

Keywords

Scattering Amplitudes; Field Theories in Higher Dimensions; Supersymmetric Gauge Theory

Funding

  1. Perimeter Institute for Theoretical Physics
  2. Government of Canada through the Department of Innovation, Science and Economic Development Canada
  3. Province of Ontario through the Ministry of Research, Innovation and Science
  4. CONICYT
  5. Royal Society University Research Fellowship [UF160350]
  6. Walter Burke Institute for Theoretical Physics at Caltech
  7. U.S. DOE [DE-SC0011632]

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We present new formulas for n-particle tree-level scattering amplitudes of sixdimensional N = (1,1) super Yang-Mills (SYM) and N = (2, 2) 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 Al = (1, 1) 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 = (2, 2) 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 SYM on the Coulomb branch.

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