High-resolution photoelectron spectroscopy using multibunch synchrotron radiation:: rotational-resolved photoelectron bands of O2+(b4Σg-,υ+)

被引:31
作者
Hsu, CW
Evans, M
Stimson, S
Ng, CY [1 ]
Heimann, P
机构
[1] Iowa State Univ, US DOE, Ames Lab, Ames, IA 50011 USA
[2] Iowa State Univ, Dept Chem, Ames Lab, Ames, IA 50011 USA
[3] Univ Calif Berkeley, Lawrence Berkeley Lab, Div Chem Sci, Berkeley, CA 94720 USA
[4] Univ Calif Berkeley, Lawrence Berkeley Lab, Adv Light Source & Accelerator & Fus Res Div, Berkeley, CA 94720 USA
关键词
D O I
10.1016/S0301-0104(97)00342-X
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
We report rotational-resolved single-photon threshold photoelectron and pulsed field ionization zero kinetic energy (PFI-ZEKE) photoelectron (PE) spectra of O-2 in the energy range of 18.1-20.2 eV measured using high-resolution monochromatized multibunch undulator synchrotron radiation. The PFI-ZEKE PE bands for O-2(+)(b (4)Sigma(g)(-) v(+) = 0-9) have been simulated using the Buckingham-Orr-Sichel model derived for rotationally resolved single-photon ionization cross-sections. Only the Delta N = - , 0 and +2 (or O, Q and S) rotational branches are observed for these PFI-ZEKE PE bands, indicating that the outgoing electron continuum channels with angular momenta l = 1 and 3 dominate in the threshold ionization transitions O-2(+)(b (4)Sigma(g)(-), v(+) = 0-9, N+) <-- O-2(X (3)Sigma(g)(-), v" = O, N"). The relative rotational branch intensities for O-2(+)(b (4)Sigma(g)(-), v(+) = 4 and 5) are found to be drastically different from those for O-2(+)(b (4)Sigma(g)(-), v(+) = 0-3, 6 and 7). Considering that the energies of O-2(+)(b (4)Sigma(g)(-), v(+) = 4 and 5) are close to the dissociation limit of O+(S-4) + O(P-3) and that the crossing location of the O-2(+)(b (4)Sigma(g)(-)) and d (4)Sigma(g)(+) potential curves is shown to be in the vicinity of O-2(+)(b (4)Sigma(g)(-), v(+) = 4 and 5), we suggest that the latter observation is thee result of predissociative perturbations by the d (4)Sigma(g)(+) state. Within the uncertainties of this experiment, the ionization energies for the formation of O-2(+)(b (4)Sigma(g)(-), v(+) = 0-9, N+ - 1) can be satisfactorily characterized using a Morse potential. The effective lifetimes for high-n Rydberg states converging to O-2(+)(b (4)Sigma(g)(-), v(+) = 0, 2-5) prepared in the present experiment are nearly constant with values in the range of 1.8-2.0 mu s The observation that the effective lifetimes for high-n Rydberg states converging to O-2(+)(b (4)Sigma(g)(-), v(+) = 4 and 5) are significantly longer than the known dissociative lifetimes of the corresponding ionic states is in accordance with the expectation that the couplings between the O-2 ion core and the high-n Rydberg electron involved are negligibly small. (C) 1998 Elsevier Science B,V. All rights reserved.
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页码:121 / 143
页数:23
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