Absolute cross sections for photoionization of excited rare gas atoms near threshold: Ar*(4p 3 D 3), Kr*(5p 3 D 3), and Xe*(6s 3 P 0) AIP Conf.The second metastable state of Kr, 5sЈ͓1/2͔ 0 , was generated from the first metastable state, 5s͓3/2͔ 2 , by optical pumping in a flow reactor. Under optimum conditions, the entire Kr͑5s͓3/2͔ 2 ͒ concentration could be removed with more than 40% conversion to the Kr͑5sЈ͓1/2͔ 0 ͒ state, which is stable in He carrier gas. The Kr͑5sЈ͓1/2͔ 0 ͒ and Kr͑5s͓3/2͔ 2 ͒ states have the Kr ϩ ͑ 2 P 1/2 ͒ and Kr ϩ ͑ 2 P 3/2 ͒ ion cores, respectively, as do the Kr ϩ X Ϫ (D) and Kr ϩ X Ϫ (B,C) states. The reactions of a series of fluorine-, chlorine-, and bromine-containing molecules, RX, with the Kr͑5sЈ͓1/2͔ 0 ͒ and Kr͑5s͓3/2͔ 2 ͒ atoms were studied by measuring the total quenching rate constants and by observing the KrX(B,C,D) product emission spectra. In contrast to the Kr͑5s͓3/2͔ 2 ͒ atoms, which give KrX͑B and C͒ products, the Kr͑5sЈ͓1/2͔ 0 ͒ atoms have a high propensity to give KrX(D) plus a lesser amount of KrX(B), depending on the reagent, as products. Discrimination against KrX(C) formation by reactions of Kr͑5sЈ͓1/2͔ 0 ͒ atoms is severe. The reactions with F 2 , NF 3 , and N 2 F 4 exhibit the highest conservation of the Kr ϩ ͑ 2 P 1/2 ͒ core, and these Kr͑5sЈ͓1/3͔ 0 ͒ reactions give Ͼ70% KrF(D). The total quenching constants of Kr͑5sЈ͓1/2͔ 0 ͒ atoms generally are equal to those for Kr͑5s͓3/2͔ 2 ͒, but the branching fractions for KrX* formation from Kr͑5sЈ͓1/2͔ 0 ͒ atoms generally are smaller than for Kr͑5s͓3/2͔ 2 ͒ atoms. A correlation diagram based on conservation of Kr ϩ ion-core state and ⍀ϭ0 Ϫ is developed to discuss these trends and the reactions of the Xe͑6sЈ͓1/2͔ 0 and 6s͓3/2͔ 2 ͒ atoms. Due to the absence of KrX(C -A) emission from the Kr͑5sЈ͓1/2͔ 0 ͒ atom reactions, the KrX(B -A) and Kr(D -A) transitions could be observed and the radiative branching ratios to the X and A states were assigned. © 1996 American Institute of Physics. ͓S0021-9606͑96͒00536-3͔ ͗ f V ͘ϭ0.6-0.7, the alignment of the rare gas halide product molecule, 3,4 and the ϳ100 Å 2 reactive cross section are typical of harpooning dynamics. 5 The corresponding Xe͑6s͓3/2͔ 1 ͒ and Kr͑5s͓3/2͔ 1 ͒ resonance atoms 6 exhibit the same reaction dynamics as the ͓3/2͔ 2 metastable atoms with X 2 molecules. For polyatomic halogen-containing molecules, RX, with smaller electron affinities than X 2 molecules, the distance at which the diabatic covalent and ion-pair potentials interact becomes smaller and ⌫ RgX* becomes less than unity, due to the competition with excitation transfer to RX* states. The ͓3/2͔ 2,1 states of Xe* and Kr* have the ground state ion core and reactions with RX molecules correlate to the rare gas halide ͑B,⍀ϭ1/2 and C,⍀ϭ3/2͒ product states, which also have the 2 P 3/2 ion-core state. The fraction of B and C molecules for different RX reagents and for Xe* vs Kr* is an aspect of the ͓3/2͔ 2,1 atom reactions that remains to be explained. In the present work, we have studied the third excited state, 5...