English

Rational Terms of UV Origin at Two Loops

High Energy Physics - Phenomenology 2020-06-24 v3 High Energy Physics - Theory

Abstract

The advent of efficient numerical algorithms for the construction of one-loop amplitudes has played a crucial role in the automation of NLO calculations, and the development of similar algorithms at two loops is a natural strategy for NNLO automation. Within a numerical framework the numerator of loop integrals is usually constructed in four dimensions, and the missing rational terms, which arise from the interplay of the (D4)(D-4)-dimensional parts of the loop numerator with 1/(D4)1/(D-4) poles in DD dimensions, are reconstructed separately. At one loop, such rational terms arise only from UV divergences and can be restored through process-independent local counterterms. In this paper we investigate the behaviour of rational terms of UV origin at two loops. The main result is a general formula that combines the subtraction of UV poles with the reconstruction of the associated rational parts at two loops. This formula has the same structure as the R-operation, and all poles and rational parts are described through a finite set of process-independent local counterterms. We also present a general formula for the calculation of all relevant two-loop rational counterterms in any renormalisable theory based on one-scale tadpole integrals. As a first application, we derive the full set of two-loop rational counterterms for QED in the RξR_{\xi}-gauge.

Keywords

Cite

@article{arxiv.2001.11388,
  title  = {Rational Terms of UV Origin at Two Loops},
  author = {Stefano Pozzorini and Hantian Zhang and Max F. Zoller},
  journal= {arXiv preprint arXiv:2001.11388},
  year   = {2020}
}

Comments

v2: Normalisation of MSbar poles clarified; v3: Version published on JHEP; References added; Further comments on use of master formula (5.61) in Sect. 6; New footnote on scale dependence in Sect. 5; Typos fixed and/or presentation improved in eqs. (4.8), (4.20), (5.2), (6.5), (6.7), (6.8), (A.2), (A.4); Results unchanged

R2 v1 2026-06-23T13:25:18.757Z