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On the Coupling of Gravitons to Matter

Z. Bern, A. De Freitas, H. L. Wong

TL;DR

Using relationships between open and closed strings, a construction of tree-level scattering amplitudes for gravitons minimally coupled to matter in terms of gauge theory partial amplitudes is presented.

Abstract

Using relationships between open and closed strings, we present a construction of tree-level scattering amplitudes for gravitons minimally coupled to matter in terms of gauge theory partial amplitudes. In particular, we present examples of amplitudes with gravitons coupled to vectors or to a single fermion pair. We also present two examples with massive graviton exchange, as would arise in the presence of large compact dimensions. The gauge charges are represented by flavors of dynamical scalars or fermions. This also leads to an unconventional decomposition of color and kinematics in gauge theories.

On the Coupling of Gravitons to Matter

TL;DR

Using relationships between open and closed strings, a construction of tree-level scattering amplitudes for gravitons minimally coupled to matter in terms of gauge theory partial amplitudes is presented.

Abstract

Using relationships between open and closed strings, we present a construction of tree-level scattering amplitudes for gravitons minimally coupled to matter in terms of gauge theory partial amplitudes. In particular, we present examples of amplitudes with gravitons coupled to vectors or to a single fermion pair. We also present two examples with massive graviton exchange, as would arise in the presence of large compact dimensions. The gauge charges are represented by flavors of dynamical scalars or fermions. This also leads to an unconventional decomposition of color and kinematics in gauge theories.

Paper Structure

This paper contains 10 equations, 3 figures.

Figures (3)

  • Figure 1: The color-ordered Feynman vertices for obtaining, via the KLT equations, gluon amplitudes dressed with gravitons. Dashed lines represent scalars and curly ones vectors.
  • Figure 2: The color-ordered Feynman diagrams contributing to $A(1_g,2_g,3_g,4_g)$.
  • Figure 3: The two diagrams contributing to the scalar partial amplitude $\tilde{A}_4(1_s^{a_1},2_s^{a_2},4_s^{a_4},3_s^{a_3})$. Each diagram is dressed with flavor group theory factors.