Abstract

We find that scattering amplitudes in massive scalar QCD can manifest the duality between color and kinematics at loop-level. Specifically we construct the one-loop integrands for four-point scattering between two distinct massive scalars, and the five-point process encoding the first correction to massive scalar scattering with gluonic radiation. We find that factorization and the color-kinematics duality are sufficient principles to entirely bootstrap these calculations, allowing us to construct all contributions ultimately from the three-point tree-level amplitudes which are themselves entirely constrained by symmetry. Double-copy construction immediately provides the associated predictions for massive scalars scattering in the so called N=0 supergravity theory.

Highlights

  • Traditional methods of calculating quantum gravitational scattering amplitudes using Feynman rules quickly run into difficulties

  • We find that scattering amplitudes in massive scalar quantum chromodynamics (QCD) can manifest the duality between color and kinematics at loop-level

  • We found the first loop correction to scattering between two different massive scalar fields, as well as the first loop correction to such scattering with an emitted gluon

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Summary

INTRODUCTION

Traditional methods of calculating quantum gravitational scattering amplitudes using Feynman rules quickly run into difficulties. In gravitational double-copy amplitudes for massive external states, even at tree level, one can generically expect the contributions of dilatons [14] This state counting and attribution naturally fits in with the states that contribute to supergravity theories, which is why the naive double-copy of pure Yang-Mills is often called N 1⁄4 0 supergravity. The highest order correction in the gravitational coupling, GN, (often called post-Minkowskian [PM]) to conservative black hole binding energy (3 PM) was only made within the past couple of years and centered amplitudes insights (see [17,58] and references therein) This calculation required the classical remnant of the two-loop four-point scattering amplitude between two massive scalars.

REVIEW
BOOTSTRAPPING TREE AMPLITUDES
Three-point trees
Four-point trees
Two massive scalars
Bootstrapping the two pairs of massive scalars four-point amplitude
One massive scalar
Five-point trees
BOOTSTRAPPING ONE-LOOP INTEGRANDS
Four-point one-loop construction
Five-point one-loop construction
Verification
CONCLUSION
Full Text
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