The role of the meson-exchange current correction to the nuclear charg
e operator is studied in electron scattering processes involving the e
xcitation of medium and heavy nuclei to energies up to the quasi-elast
ic peak. The effect of these contributions in the quasi-free electron
scattering process is a reduction of at most a 3% in the longitudinal
response at the energy of the peak, a value which is below the experim
ental error and must not be taken into account in calculations in this
energy region. On the other hand, the excitation of low-lying nuclear
levels of neutronic character shows, with respect to the protonic one
s, a considerable effect due to the inclusion of the two-body term in
the charge operator. More realistic calculations, such as those perfor
med in the random-phase approximation framework, give rise to a mixing
of one particle-one hole configurations of both kinds which reduce th
ese effects. However, it has been found that the excitation of some of
these levels is sizably affected by the meson-exchange contribution.
More precise experimental data concerning some of these states, such a
s e.g. the high-spin states in Pb-208, could throw some light in the p
roblem of a more feasible determination of these effects and, as a con
sequence, could provide an alternative procedure to determine the char
ge neutron form factor. (C) 1997 Elsevier Science B.V.