A relativistic Green's function approach to parity-violating quasielastic
electron scattering is presented. The components of the hadron tensor are
expressed in terms of the single particle Green's function, which is expanded
in terms of the eigenfunctions of the non-Hermitian optical potential, in order
to account for final state interactions without any loss of flux. Results for
12C, 16O, and 40Ca are presented and discussed. The effect of
the strange quark contribution to the nuclear current is investigated.Comment: 24 pages, 13 figure