The 248 nm photodissociation of KI: Determination of the branching ratio of K(42 P J ) doublets in the presence of Ar, H2, and N2 J. Chem. Phys. 99, 9603 (1993); 10.1063/1.465493Ultraviolet absorption cross sections for N2H4 vapor between 191-291 nm and H(2 S) quantum yield in 248 nm photodissociation at 296 K S4 N4 was photolyzed by the KrF excimer laser source at 248 nm. The excited state photofragments produced are the NS(B 211) rand NS(H 211) 1/2' NS( G 2~ -) and NS(l2~ + ) states. Single band progression fluorescence out of v' = 0 for NS (H) 1/2 and v' = 2 for NS (G,/) are observed. Franck-Condon factors have been calculated for NS(H). up to v' = 3. The electronic transition moment for the NS(H-X) transition was found to decrease slightly with increasing r. The radiative lifetime of the 0,5 band ofNS(H) 112 is determined to be 87 + 11 ns.The collisional quenching constants at 335 K for various species including N2 -(k q = 3.4 ± 0.7 X 10-10 cm 3 s -1), CF 4 (k q = 1.8 ± 0.4 X 10-10 cm 3 s -1), SF 6 (k q = 3.9 ± 0.7X 10-10 cm 3 s -1) and He (k q = 5.6 ± 2.2x 10-11 cm 3 s -1) are reported. A semiempirical calculation using a PM3 Hamiltonian was used to calculate the heats of formation of various (SN) x species. A mechanism is proposed to account for the presence of these excited states based on laser fluence, excited state time histories, spectral composition and calculated heats of formation. NS(B) is postulated to arise directly from an intermediate photolysis product which is assumed to be acyclic S3 N 3' The NS (H 211) 1/2 subband, NS( G 2~ -) and NS(l2~ + ) states are thought to be produced from a resonant interaction with the KrF line at 248 nm and vibrationally excited ground state NS. Using the 12 (D i g -A iu ) emission as an actinometer, the overall efficiency on the conversion of absorbed photons by S4N4 into NS(B 2n) is 2.6 ± 0.7%. M Sep) + N(4S) + M --+NS(a 411)~NS(b 4~ -) M --+NS(B 2IT),