Higher-order corrections to the two and three-fermion Salpeter equations

TL;DR

This paper compares two methods for reducing the Bethe-Salpeter equation to three-dimensional form and extends these ideas to derive first-order energy corrections for three-fermion systems.

Contribution

It introduces a new approach to three-fermion Bethe-Salpeter equations based on propagator-approximated reductions, providing a way to compute energy corrections.

Findings

Kernel-approximated reduction does not yield correct scattering amplitudes.

The derived 3D equations enable calculation of first-order energy corrections.

The approach simplifies the complex three-fermion Bethe-Salpeter equation.

Abstract

We compare two opposite ways of performing a 3D reduction of the two-fermion Bethe-Salpeter equation beyond the instantaneous approximation and Salpeter's equation. The more usual method consists in performing an expansion around an instantaneous approximation of the product of the free propagators (propagator-approximated reduction). The second method starts with an instantaneous approximation of the Bethe-Salpeter kernel (kernel-approximated reduction). In both reductions the final 3D potential can be obtained by following simple modified Feynman rules. The kernel-approximated reduction, however, does not give the correct scattering amplitudes, and must thus be limited to the computation of bound states. Our 3D reduction of the three-fermion Bethe-Salpeter equation is inspired by these results. We expand this equation around positive-energy instantaneous approximations of the three two-body kernels, but these starting approximations are given by propagator-approximated reductions at the two-body level. The three-fermion Bethe-Salpeter equation is first transformed into a set of three coupled equations for three wave functions depending each on one two-fermion total energy, then into a set of three 3D equations and finally into a single 3D equation. This last equation is rather complicated, as it combines three series expansions, but we use it to write a manageable expression of the first-order corrections to the energy spectrum.