In a weak magnetic field coherent dark resonances in cesium vapor are
split into up to 15 resolved components, depending on field direction
and laser polarizations. We find that the selection rules are differen
t for vapor cells with and without buffer gas due to a change in multi
polarity of the two-photon coupling. At low laser intensities or suffi
ciently high buffer-gas pressure optical pumping between different dar
k resonances can be neglected so that a simple model allows one to cal
culate the relative line strengths, giving complete agreement with the
experimental spectra.