The off-shell two-loop correction to the massive quark propagator in an
arbitrary covariant gauge is calculated and results for the bare and
renormalized propagator are presented. The calculations were performed by means
of a set of new generalized recurrence relations proposed recently by one of
the authors. From the position of the pole of the renormalized propagator we
obtain the relationship between the pole mass and the MS mass. This
relation confirms the known result by Gray et al.. The bare amplitudes are
given for an arbitrary gauge group and for arbitrary space-time dimensions.(more)
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%0 Journal Article
%1 Fleischer1999Twoloop
%A Fleischer, J.
%A Jegerlehner, F.
%A Tarasov, O. V.
%A Veretin, O. L.
%D 1999
%J Nuclear Physics B
%K renormalised\_mass, two-loop
%N 3
%P 671--690
%R 10.1016/S0550-3213(98)00705-6
%T Two-loop QCD corrections of the massive fermion propagator
%U http://dx.doi.org/10.1016/S0550-3213(98)00705-6
%V 539
%X The off-shell two-loop correction to the massive quark propagator in an
arbitrary covariant gauge is calculated and results for the bare and
renormalized propagator are presented. The calculations were performed by means
of a set of new generalized recurrence relations proposed recently by one of
the authors. From the position of the pole of the renormalized propagator we
obtain the relationship between the pole mass and the MS mass. This
relation confirms the known result by Gray et al.. The bare amplitudes are
given for an arbitrary gauge group and for arbitrary space-time dimensions.
@article{Fleischer1999Twoloop,
abstract = {The off-shell two-loop correction to the massive quark propagator in an
arbitrary covariant gauge is calculated and results for the bare and
renormalized propagator are presented. The calculations were performed by means
of a set of new generalized recurrence relations proposed recently by one of
the authors. From the position of the pole of the renormalized propagator we
obtain the relationship between the pole mass and the \bar{MS} mass. This
relation confirms the known result by Gray et al.. The bare amplitudes are
given for an arbitrary gauge group and for arbitrary space-time dimensions.},
added-at = {2014-01-09T15:14:33.000+0100},
archiveprefix = {arXiv},
author = {Fleischer, J. and Jegerlehner, F. and Tarasov, O. V. and Veretin, O. L.},
biburl = {https://www.bibsonomy.org/bibtex/2be6e56255e398f78f162d0ccbd62893f/jaspervh},
citeulike-article-id = {7722527},
citeulike-linkout-0 = {http://dx.doi.org/10.1016/S0550-3213(98)00705-6},
citeulike-linkout-1 = {http://arxiv.org/abs/hep-ph/9803493},
citeulike-linkout-2 = {http://arxiv.org/pdf/hep-ph/9803493},
citeulike-linkout-3 = {http://dx.doi.org/10.1016/S0550-3213(98)00705-6},
comment = {Relation between bare and two-loop renormalised mass.},
day = 20,
doi = {10.1016/S0550-3213(98)00705-6},
eprint = {hep-ph/9803493},
interhash = {96dcf7624159eefb5bc3c305cc22153e},
intrahash = {be6e56255e398f78f162d0ccbd62893f},
issn = {05503213},
journal = {Nuclear Physics B},
keywords = {renormalised\_mass, two-loop},
month = sep,
number = 3,
pages = {671--690},
posted-at = {2010-08-27 16:02:05},
priority = {2},
timestamp = {2014-01-09T15:14:33.000+0100},
title = {Two-loop QCD corrections of the massive fermion propagator},
url = {http://dx.doi.org/10.1016/S0550-3213(98)00705-6},
volume = 539,
year = 1999
}