We calculate the Coulomb displacement energies (CDEs) of mirror nuclei usin
g the recent parameter set (NL3) in the relativistic mean-field (RMF) model
which includes self-coupling of the scalar meson. The results obtained are
compared with the available ones calculated in the nonrelativistic Skyrme-
Hartree-Fock (SHF) approach that have the best fit to the experimental data
. When adjusted to reproduce the charge root-mean-square (rms) radius r(c)
and the rms radii of the valence orbits, the results of the RMF model for t
he CDEs agree with those of the SHF model within similar to 1 %. Our invest
igation also shows that, although the RMF with the NL3 parameter set reprod
uces the kink in the isotope variation of r(c), the values obtained for CDE
s are too small to account for the experimental values without the addition
of the contribution due to long-range correlation effects.