It is shown that conventional mass renormalization, when applied to ph
otonic or gluonic corrections to unstable particle propagators, leads
to non-convergent series in the resonance region. A solution of this p
roblem, based on the concepts of pole mass and width, is presented. In
contrast with the Z case, the conventional on-shell definition of mas
s for W bosons and unstable quarks contains an unbounded gauge depende
nce in next-to-leading order. The on-shell and pole definitions of wid
th ale shown to coincide if terms of O(Gamma(2)) and higher are neglec
ted, but not otherwise.