Abstract:Experimental ratios of branching in the fine-structure levels of the Rb5P multiplet, as a consequence of an optical collision with He, are reported. The process studied is Rb(5S1/2)+He+hν→Rb(5PJ)+He, where the pulsed laser frequency ν is tuned in the wings of the Rb resonance transitions. The authors defined the detuning Δ to be ν-ν(D2)(Δ>0) for laser frequency ν highter than that of RbD2 transition and to be ν-ν(D1)(Δ<0) for ν lower than the RbD1 transition. As RbHe molecular states are correlated to the two 5 2PJ states, there is some likelihood that the molecule will dissociate into 5 2P1/2 or 5P3/2 state. The dissociation results in a nonuniform distribution of atomic Rb5PJ states. The branching ratios are defined as n1/n2, where n1 and n2 are densities of the 5P1/2 and 5P3/2 states dissociated. To determine experimentally the relative cross section for scattering into the two fine-structure states, the relative time-intergrated intensities of the resulting Rb emission lines, I(5P3/2→5P1/2)[I(D2)] and I(5P1/2→5P3/2)[I(D1)] , were measured. The ratios are determined by detunings from about 200 cm-1 in the blue wing to -180 cm-1 in the red wing of the Rb5P multiplet. A rate equation analysis of the pressure dependence was yielded. The branching ratios and cross sections for collisional 5P1/2→5P3/2 transition were obtained from the slope and intercept. The blue-wing branching ratios show a detuning-dependent approach to limit of 0.2. The branching was found to be very large (~40) in the red wing, irrespective of the detuning. Fine structure changing cross section (1.1±0.3)×10-17 cm2 was measured from wing excitation, and the result is consistent with the cross section obtained from resonant excitation of the Rb5PJ state. The measurements show a strong sensitivity to interatomic potentials and to nonadiabatic effects in dissociation dynamics.
[1] Havey M D, Delahanty F T, Vahala L L, et al. Phys. Rev., 1986, A34(4): 2758. [2] Vahala L L, Julienne P S, Havey M D. Phys. Rev.,1986, A34(3):1856. [3] Goldstein R, Grosser J, Hoffmann O, et al. J. Chem. Phys.,2001, 114(5): 2144. [4] Figl C, Goldstein R, Grosser J, et al. J. Chem. Phys.,2004, 121(22):11068. [5] SHEN Yi-fan, LI Wan-xing(沈异凡,李万兴). Spectroscopy and Spectral Analysis(光谱学与光谱分析),2001,21(1):38. [6] Schaty G C, Hanhel T W, Whiteley W J, et al. J. Phys. Chem., 2003, A107: 7278. [7] Ermers A, Woschnih T, Behmenburg B. Z. Phys., 1987, D5: 113. [8] Grosser J,Hoffmann O, Wischeler F S, et al. J. Chem. Phys., 1999, 111: 2853. [9] Habitg P. Chem. Phys., 1980, 54: 131. [10] Botschwina P, Meyer W, Hertel I V, et al. J. Chem. Phys., 1981, 75: 5438. [11] Theodosiou C E. Phys. Rev., 1984, A30(6): 2881. [12] Gallagher A, Lewis E L. J. Opt. Soc. Am., 1973, 63(7): 864. [13] Gallagher A. Phys. Rev., 1968, 172: 88. [14] Cuvellier J, Fournier P R, Gounand F, et al. Phys. Rev., 1975,A11(3): 846. [15] Vadla C, Knezovic S, Movre M. J. Phys., 1992, B25: 1337.