1999
DOI: 10.1016/s0301-0104(99)00077-4
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E0g+→A1u and E0g+→B″1u laser-induced fluorescence in molecular iodine recorded by Fourier-transform spectroscopy

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Cited by 31 publications
(28 citation statements)
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“…It can be seen that the R:Q:P branch ratios are not 1:2:1 as expected, with the P branch (J = 31 → 32 emission line) being significantly more intense than the R branch. This phenomenon can be observed in the spectra shown by Inard et al 2 but was not commented on by the authors. In all of the spectra that we recorded, the trend increases with J; two examples are shown in Figs.…”
Section: B R:q:p Branch Ratios In E0 Gmentioning
confidence: 83%
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“…It can be seen that the R:Q:P branch ratios are not 1:2:1 as expected, with the P branch (J = 31 → 32 emission line) being significantly more intense than the R branch. This phenomenon can be observed in the spectra shown by Inard et al 2 but was not commented on by the authors. In all of the spectra that we recorded, the trend increases with J; two examples are shown in Figs.…”
Section: B R:q:p Branch Ratios In E0 Gmentioning
confidence: 83%
“…2 It could be clearly seen that while the P:Q:R branch ratios in the direct E0 g + ( 3 P 2 ) → C1 u emission were as expected, those in the E0 g + ( 3 P 2 ) → A1 u emission were not, but this observation was not commented on by the authors. In this case, we will propose that the imbalance is due to -uncoupling between the E0 g + ( 3 P 2 ) and β1 g ( 3 P 2 ) states, first reported in absorption by Perrot et al 4 Potential energy curves of all of the relevant states 2, 5-10 are shown in Fig.…”
Section: Introductionmentioning
confidence: 83%
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“…In another OODR study [16] in which two continuous-wave dye lasers were used, (v = 1) of the E0 þ g ð 3 P 2 Þ state was excited and transfer induced by collisions with I 2 in the ground state observed. The simulations of the D0 þ u ð 3 P 2 Þ !…”
Section: Vibrational Distribution Following Ase and Collisional Energmentioning
confidence: 99%