Abstract

We compute the leading post-Newtonian and quantum corrections to the Coulomb and Newtonian potentials using the full modern arsenal of on-shell techniques; we employ spinor-helicity variables everywhere, use the Kawai-Lewellen-Tye (KLT) relations to derive gravity amplitudes from gauge theory and use unitarity methods to extract the terms needed at one-loop order. We stress that our results are universal and thus will hold in any quantum theory of gravity with the same low-energy degrees of freedom as we are considering. Previous results for the corrections to the same potentials, derived historically using Feynman graphs, are verified explicitly, but our approach presents a huge simplification, since starting points for the computations are compact and tedious index contractions and various complicated integral reductions are eliminated from the onset, streamlining the derivations. We also analyze the spin dependence of the results using the KLT factorization, and show how the spinless correction in the framework are easily seen to be independent of the interacting matter considered.

Highlights

  • Of the theory [6,7,8,9,10,11,12,13,14]

  • We compute the leading post-Newtonian and quantum corrections to the Coulomb and Newtonian potentials using the full modern arsenal of on-shell techniques; we employ spinor-helicity variables everywhere, use the Kawai-Lewellen-Tye (KLT) relations to derive gravity amplitudes from gauge theory and use unitarity methods to extract the terms needed at one-loop order

  • The unitarity cut for the leading quantum corrections involves the gravitational Compton amplitude, i.e. the two on-shell gravitons coupled to matter

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Summary

The gravitational Compton amplitude

We will do this first using covariant amplitudes, and more compactly using the helicity formalism. The advantage of this approach is that one can use the known expressions for the massive tree-level amplitudes in Yang-Mills and QED to obtain in a condensed way the massive tree-level amplitudes in gravity.

Covariant notation
Massive trees amplitude in gravity from Yang-Mills tree amplitudes
The QED amplitudes
The gravity amplitudes
The one-loop amplitude in the helicity formalism
The one-loop correction to Coulomb potential
The one-loop correction to Newton potential
The one-loop amplitude in harmonic gauge
Comparison with the Feynman graph approach
Matter universality of the quantum corrections
The spin 1 case
Conclusion
A Vertices and propagators
B Dispersion relations
Full Text
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