General properties of logarithmically divergent one-loop lattice Feynman integrals

dc.creatorKim, Jongjeong
dc.creatorAdams, David H.
dc.creatorLee, Weonjong
dc.date2007-10-10
dc.date.accessioned2026-07-07T13:02:51Z
dc.date.available2026-07-07T13:02:51Z
dc.descriptionWe prove that logarithmically divergent one-loop lattice Feynman integrals have the general form I(p,a) = f(p)log(aM)+g(p,M) up to terms which vanish for lattice spacing a -> 0. Here p denotes collectively the external momenta and M is an arbitrary mass scale. The f(p) is shown to be universal and to coincide with the analogous quantity in the corresponding continuum integral (regularized, e.g., by momentum cut-off). This is essential for universality of the lattice QCD beta-function and anomalous dimensions of renormalized lattice operators at one loop. The result and argument presented here are simplified versions of ones given in arXiv:0709.0781. A noteworthy feature of the argument here is that it does not involve Taylor expansion in external momenta, hence infra-red divergences associated with that expansion do not arise.
dc.description7 pages, presented at the XXV International Symposium on Lattice Field Theory, July 30 - August 4 2007, Regensburg
dc.identifierhttps://arxiv.org/abs/0710.1930
dc.identifierhttp://arxiv.org/abs/0710.1930
dc.identifierPoSLAT2007:266,2007
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/226593
dc.subjectHigh Energy Physics - Lattice
dc.titleGeneral properties of logarithmically divergent one-loop lattice Feynman integrals
dc.typetext

Files

Collections