The cross sections of spin-orbit energy exchange between the cesium 6 2 P 1/2 ↔ 6 2 P 3/2 states induced by collisions with N 2 , H 2 , HD, D 2 , CH 4 , C 2 H 6 , CF 4 , and C 2 F 6 were obtained for pressures less than 100 Torr at room temperature by means of steady-state laser-induced fluorescence techniques. The spin-orbit energy exchange rate with N 2 , H 2 , HD, D 2 , CH 4 , C 2 H 6 , CF 4 , and C 2 F 6 , have been measured as σ 21 (6 2 P 3/2 → 6 2 P 1/2 ) = 16. 3, 34.1, 30.0, 22.7, 21.4, 65.6, 64.8, and 137Å 2 and σ 12 (6 2 P 1/2 → 6 2 P 3/2 ) = 1. 8, 4.4, 4.1, 3.0, 2.9, 13.3, 9.7, and 16.3Å 2 , respectively. Correlations of the spin-orbit transfer probabilities with rotational-energy defect and vibrational-energy defect have been shown.