We evaluate the coefficients of the leading poles of the complete two-loop
quark self-energy Sigma (p) in the Coulomb gauge. Working in the framework
of split dimensional regularization, with complex regulating parameters sig
ma and n/2 - sigma for the energy and space components of the loop momentum
, respectively, we find that split dimensional regularization leads to well
-defined two-loop integrals, and that the overall coefficient of the leadin
g pole term for Sigma (p) is strictly local. Extensive tables showing the p
ole parts of one- and two-loop Coulomb integrals are given. We also comment
on some general implications of split dimensional regularization, discussi
ng in particular the limit sigma --> 1/2 and the subleading terms in the E-
expansion of noncovariant integrals. (C) 2000 Elsevier Science B.V. All rig
hts reserved.