We have reinvestigated the \(0_{u}^{+}\left({ }^{3} P_{0}\right)\) ion-pair state of \(\mathrm{Cl}_{2}\) correlating to \(\mathrm{Cl}^{-}\left({ }^{1} S\right)+\mathrm{Cl}^{+}\left({ }^{3} P_{0}\right)\) by optical-optical double resonance. The \(\mathrm{Cl}_{2}\) molecules in the \(X^{1} \Sigma_{g}
Optical-Optical Double-Resonance Spectroscopy of the I2 0+g(1D) Ion-Pair State
✍ Scribed by T. Ishiwata; J. Yamada; K. Obi
- Publisher
- Elsevier Science
- Year
- 1993
- Tongue
- English
- Weight
- 394 KB
- Volume
- 158
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
The (0_{g}^{+}\left({ }^{1} D\right)) ion-pair state of (\mathrm{I}{2}) has been analyzed by optical-optical double-resonance using the (0{g}^{+}\left({ }^{1} D\right)-B^{3} \Pi\left(0_{u}^{+}\right)-X^{1} \Sigma_{g}^{+})photoexcitation sequence. The analysis of the 374 transitions in the (0 \leqslant v \leqslant 20) and (9 \leqslant J \leqslant 117) range yields a set of molecular parameters in a Dunham-lype expansion: (Y_{00}=55409.954(3), Y_{10}=97.0979(11), Y_{20}=-0.19360(12), Y_{30}=2.781(35) \times) (10^{-4}, Y_{01}=0.01815891(64), Y_{11}=-3.362(12) \times 10^{-5}, Y_{21}=-1.65(66) \times 10^{-8}), and (Y_{02}=) (-2.639(40) \times 10^{-9}) (all in (\mathrm{cm}^{-1}) and (\sigma) in parentheses). An RKR potential is constructed based on these constants, and used to interpret the (0_{g}^{+}\left({ }^{1} D\right)-B^{3} \Pi\left(0_{u}^{+}\right))emission. We also observed a highly vibrational excited (0_{g}^{+}\left({ }^{3} P_{0}\right)) state, whose molecular constants valid up to (v=101) are reported. (c) 1993 Academic Press. Inc.
📜 SIMILAR VOLUMES
We have analyzed the 1 u ( 1 D) and 2 u ( 1 D) ion-pair states of I 2 by perturbation-facilitated optical-optical double resonance using the B 3 (0 + u ) ∼ c1 g mixing state as an intermediate. The double-resonance spectra exhibited the strong vibrational progression to the 1 u ( 1 D) state in accor
We have reexamined the sequential two-photon absorption of I 2 from the X 1 + g ground state to the lowest D 2 g ( 3 P 2 ) ionpair state using the high vibrational level of the B 3 (0 + u ) state as an intermediate. The double resonance transition to the D 2 g ( 3 P 2 ) state was found to occur thro
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