first-order perturbations including S-O couplings are accounted for. The calculated molecular constants are in reasonable agreement with the experimental ones. The calculated lanthanide contractions of the three series, i.e. R(La-X) -R(Lu-X), are quite different, 0.19 Á (0.19 Á) for LnH, 0.10 Á (0.11 Á) for LnF, and only 0.05 Á (0.04 Á) for LnO.There is good agreement between the calculated values and the experimental ones (values in parentheses). This astonishing variation has two origins, a monoatomic and a diatomic one, which are related to each (DW), spin-orbit (SO), and so-called indirect core effects (DVC). The cores are treated at the Dirac-Fock-Slater level.LnH, LnF, and LnO have been calculated in their ground configurations. In general, the lanthanides are trivalent;27 i.e., the valence configuration is f with N = 0,7, and 14 for La, Gd, and Lu, respectively. But for Yb (N = 13) also the divalent state is common, with occupied f-v+1=14 shell. The superconfigurations of the ground states in general are: (4 ) 2 2 for LnH, (4 ) 2 2 2 3 4 for LnF and (4 ) 2 2 , 4 for LnO.However, there are exceptions. Concerning the Yb compounds, the ground configurations are (4f14)a2a1 for YbH, (4 ,4) 2 2 4 for YbF, and (4 14) 2 2 2 4 for YbO. The significant (4 3) 2 2 1 4 ' + admixture in the YbO ground state12 has been neglected here except where explicitly noted. Another exception is LaH: 4 ° 2 2 represents one of the low-lying excited states.