Bound and quasibound states of the NaFH van der Waals moleculeFor the open shell van der Waals molecule, CAr, the potential energy curves ͑PECs͒ for the B 3 ⌸ and 1 5 ⌺ Ϫ states, the B 3 ⌸ -1 5 ⌺ Ϫ spin-orbit coupling and the B 3 ⌸ fine structure splitting are determined using multireference configuration interaction wave functions as large as ϳ8 million configuration state functions. The B 3 ⌸ state is strongly bound, with D e ϭ5100 cm Ϫ1 . R e (B 3 ⌸) ϭ3.7a 0 and is considerably shorter than R e (X 3 ⌺ Ϫ )ϭ6.07 a 0 . The PEC for the repulsive 1 5 ⌺ Ϫ state crosses that of the B 3 ⌸ state at R x (1 5 ⌺ Ϫ ,B 3 ⌸)ϭ3.31a 0 leading to spin-orbit induced predissociation. The B 3 ⌸ -1 5 ⌺ Ϫ spin-orbit coupling is the result of valence-Ryberg mixing in the B 3 ⌸ state and is considerably enhanced by the heavy atom effect. The heavy atom effect is also reflected in a marked decrease in the fine structure splitting of the B 3 ⌸ state with increasing vibrational level. The implications of these results for using CAr(B 3 ⌸) in laser induced fluorescence detection of CAr(X 3 ⌺ Ϫ ,v) are discussed.