EVIDENCE FOR PREDISSOCIATION OF $Rb^{*}_{2}(C^{1}\Pi_{u})$ INTO $Rb^{*}(^{2}P_{3/2})$ AND $Rb(^{2}S_{1/2})$

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1976

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Ohio State University

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A nozzle beam of rubidium is irradiated by the 4765 {\AA} line of the argon ion laser, and the resulting fluorescence is spectroscopically analyzed. Under these collision-free conditions, the emission consists of molecular fluorescence from the Rb2C1ΠuX1Σg+ electronic system as well as atomic fluorescence from the Rb 2P3/2 fine structure component (the Rb D2 line) only. The latter transition is caused by partial predissociation (≤25 of the Rb2C1Πu state.1 The molecular fluorescence is polarized and has a value P=0.345±0.009. This is interpreted to be caused by the superposition of P and R2 as well as Q lines, in agreement with studies made by Happer and Tam.2 The Rb 52P3/2 level correlates with the Rb2A1Σu+ state or the B1Πu state, one or both of which are believed to be responsible for predissociating the Rb2C1Πu state.

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1J. M. Brom and H. P. Broida, J. Chem. Phys. 61, 982 (1974). 2A. Tam and W. Happer, submitted to the Journal of Chemical Physics.


Author Institution: Department of Chemistry, Columbia University, New York

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