Abstract

An electron spectrometric study has been performed on HBr using metastable helium and neon atoms as well as helium resonance photons. High resolution electron spectra were obtained for a mixed He(21S, 23S) beam, a pure He(23S) beam, a mixed Ne(3s3P2,3P0) beam, and for HeI VUV light. From the comparison of vibrational populations of HBr+ (X, v′) and HBr+ (A, v′), formed by either He* and Ne* Penning ionization (PI) or HeI photoionization, we conclude that HBr+ (X) formation by PI exhibits only little perturbation of HBr potentials, whereas HBr+ (A) formation by PI exhibits substantial bond stretching of HBr due to metastable atom attack preferably from the H end. For He(21S) + HBr theX- andA-state vibrational peak shapes are substantially broader than for the He(23S) + HBr case pointing to an additional, charge exchanged interaction (He+ + HBr−) in the entrance channel of the former system which is also responsible for a broad feature found at lower electron energies in the He(21S, 23S) induced PI electron spectra. For the first time, we have detected the low energy electrons in both the He(21S) + HBr and He(23S) + HBr spectra, associated with the major mechanism for the formation of Br+ ions: energy transfer to repulsive HBr** Rydberg states, dissociating to H(1s) and autoionizing Br** atoms. The HBr+ (X)2II3/2:2II1/2 fine structure branching ratios vary significantly with the ionizing agent in a similar way as for the isoelectronic, atomic target case krypton.

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