The difference R(z) between the resolvents of the interacting and free
Hamiltonians is inherently associated with (pair) particle correlatio
ns and can also be used for the evaluation of the second virial coeffi
cient. This paper explores the operator properties of R(z) and the ana
lytical continuation of its momentum matrix elements. Correlated-state
wave functions are identified when making a pole expansion of the ana
lytically continued matrix elements. These square-integrable wave func
tions have a one-to-one correspondence with resolvent poles, and as su
ch are associated with resonance-bound-, and virtual-state momenta. Th
eir properties and use in evaluating the second virial coefficient are
discussed. Except for the bound states, these wave functions are not
eigenvectors of the interacting Hamiltonian. The separable Yamaguchi p
otential is used to illustrate these properties.