The interaction of He(2 3 S) with CS 2 produces relatively strong emission from the CS + (A 2 II−X 2 ∑ + ) and CS(A 1 II−X 1 ∑ + ) systems; weaker emission is observed from CS 2 + (A 2 II u −X 2 II g ), CS 2 + (B 2 ∑ u + −X 2 II g ), CS(a 3 II−X 1 ∑ + ), some unassigned transitions, and atomic emission (mainly from S * ) in the vacuum ultraviolet. Several new CS + (A−X) emission bands were observed and these yield improved spectroscopic constants for both the CS + (X) and CS + (A) states. Available data for Δ H fo Q (CS) are critically assessed, and estimates of Δ H fo Q (CS + )=326.4±0.7 and D 0 0 (CS + )=147.8±0.9 kcal mole −1 are obtained. The experimentally observed band intensities were combined with Franck-Condon factors calculated from a Morse potential for CS + (X) and an RKR potential for CS + (A) to obtain vibrational populations, and to compare calculated and experimental radiative branching ratios. The band intensities from the CS(A 1 II, v ′=0–4) levels were combined with calculated RKR Franck-Condon factors to analyze the dependence of the electronic transition moment on r-centroid. The other emission systems observed from the He(2 3 S)+CS 2 reaction also are summarized, and some aspects of the quenching mechanism are discussed and compared to the photoionization of CS 2 .