Two-Loop Quark Self-Energy in a New Formalism: (I) Overlapping Divergences

TL;DR

The paper introduces a novel matrix method for evaluating multi-loop Feynman integrals, effectively handling divergences in two-loop quark self-energy calculations within light-cone gauge, applicable to various gauges and integral types.

Contribution

A new matrix method for multi-loop Feynman integrals is developed, enabling exact analytic evaluation of divergences in complex gauge calculations, including noncovariant gauges.

Findings

The method confirms existing divergence results in the Standard Model.

It simplifies the evaluation of covariant and noncovariant gauge integrals.

The technique is applicable to both massive and massless integrals.

Abstract

A new integration technique for multi-loop Feynman integrals, called the matrix method, is developed and then applied to the divergent part of the overlapping two-loop quark self-energy function $\,i\Sigma\,$ in the light- cone gauge. It is shown that the coefficient of the double-pole term is strictly local, even off mass-shell, while the coefficient of the single-pole term contains local as well as nonlocal parts. On mass-shell, the single-pole part is local, of course. It is worth noting that the original overlapping self-energy integral reduces eventually to 10 covariant and 38 noncovariant- gauge integrals. We were able to verify explicitly that the divergent parts of the 10 double covariant-gauge integrals agreed precisely with those currently used to calculate radiative corrections in the Standard Model. Our new technique is amazingly powerful, being applicable to massive and massless integrals alike, and capable of handling both covariant-gauge integrals and the more difficult noncovariant-gauge integrals. Perhaps the most important feature of the matrix method is the ability to execute the $4\omega$-dimensional momentum integrations in a single operation, exactly and in analytic form. The method works equally well for other axial-type gauges, notably the temporal gauge ($n^2>0$) and the pure axial gauge ($n^2<0$).