  The Coulomb gauge in nonabelian gauge theories is attractive in principle,
but beset with technical difficulties in perturbation theory. In addition to
ordinary Feynman integrals, there are, at 2-loop order, Christ-Lee (CL) terms,
derived either by correctly ordering the operators in the Hamiltonian, or by
resolving ambiguous Feynman integrals. Renormalization theory depends on the
subgraph structure of ordinary Feynamn graphs. The CL terms do not have
subgraph structure. We show how to carry out enormalization in the presene of
CL terms, by re-expressing these as `pseudo-Feynman' inegrals. We also explain
how energy divergences cancel.
