Abstract
Fluorescence from excited alkali atoms (A*) may be produced by photodissociation of alkali halide (AX) vapor. Fluorescence efficiencies have been determined as a function of the photodissociation wavelength, λ0, for Na* (3 2P) from NaBr and for K* (4 2P) and K* (5 2P) from KI. Employing the Stern‐Volmer relation, cross sections, Qq, for the collisional quenching of the A* electronic excitation may be determined from the attenuation of the A* fluorescence that is observed upon introduction of a foreign gas. Because A* may be produced with different average speeds by varying λ0, this method permits the determination of the dependence of Qq on relative collision speed, g. Employing this method, Qq was determined to decrease monotonically with increasing g for Na* (3 2P)+Br2 (AX = NaBr) and K* (4 2P)+C2H4, CF3Cl, and SO2 (AX = KI). Moreover, values of Qq were determined at a particular g value for K* (4 2P)+I2 and K* (5 2P)+I2, HCl, and DCl. Alternatively, premixing the quenching gas in a large (∼ 100‐fold) excess of Ar thermal moderator (Ar failed to quench any of these A* levels) makes possible the measurement of Qq for a thermal distribution in g. Thermal results (800–900°K) obtained by this method are reported for the quenching of Na* (3 2P) (AX=NaI), K* (4 2P), and/or K* (5 2P) by N2, CF3Cl, H2, H2O, CH3OH, CF4, CH4, C2H6, C2H4, and SO2. In general, for any particular quenching gas, Qq[K* (5 2P)] > Qq[Na* (3 2P)] ≳ Qq[K* (4 2P)] . The difference between K* (52P) and K* (4 2P) [or Na* (3 2P)] is sometimes quite large; for CH4, for example, Qq[K* (5 2P)]/Qq[K* (4 2P)] > 60. For I2, however, the trend is dramatically reversed with Qq[K* (5 2P)]/Qq[K* (4 2P)]=0.2. Effects of isotopic substitution were also examined; no difference in Qq was measured for H2 vs D2, H2O vs D2O, C2H4 vs C2D4, or HCl vs DCl. However, for K* (5 2P), Qq(CH4)/Qq(CD4) ≈ Qq(C2H6)/Qq(C2D6) ≈ √2. All of these results are discussed in terms of the likely forces between the reactants and the possibility of a change‐transfer intermediate.

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