We use a gauge-invariant regularization procedure, called split dimens
ional regularization, to evaluate the quark self-energy Sigma(p) and q
uark-quark-gluon vertex function Lambda(mu) (p',p) in the Coulomb gaug
e, del.A(a) = 0. The technique of split dimensional regularization was
designed to regulate Coulomb-gauge Feynman integrals in non-Abelian t
heories. The technique which is based on two complex regulating parame
ters, omega and sigma, is shown to generate a well-defined set of Coul
omb-gauge integrals, A major component of this project deals with the
evaluation of four-propagator and five-propagator Coulomb integrals, s
ome of which are non local. It is further argued that the standard one
-loop BRST identity relating Sigma and Lambda(mu), should by rights be
replaced by a more general BRST identity which contains two additiona
l contributions from ghost vertex diagrams. Despite the appearance of
non-local Coulomb integrals, both Sigma and Lambda(mu), are local func
tions which satisfy the appropriate BRST identity. Application of spli
t dimensional regularization to two-loop energy integrals is briefly d
iscussed. (C) 1998 Elsevier Science B.V.