1996年7月22日
High-resolution laser spectroscopy of the X1Σ+ and (1)3Σ+ states of 23Na85Rb molecule
Journal of Chemical Physics
- ,
- ,
- ,
- ,
- ,
- ,
- 巻
- 105
- 号
- 4
- 開始ページ
- 1341
- 終了ページ
- 1347
- 記述言語
- 英語
- 掲載種別
- DOI
- 10.1063/1.472000
- 出版者・発行元
- American Institute of Physics Inc.
High-resolution spectra of the B1Π→X1Σ+ transition of 23Na85Rb molecule are measured by the technique of the Doppler-free optical-optical double resonance polarization spectroscopy (OODRPS). The molecular constants of the X1Σ+(v″=5-30) levels are determined, and the potential energy curve is constructed up to v″=30 by the RKR method. The time-resolved fluorescence intensity following the excitation to the B1Π(v′=5,J′= around 20) level is measured, and the lifetime of the B1Π(v′=5) level in collisionless limit is determined to be 17.8 ns. The absolute value of the electric dipole moment of the B1Π-X1Σ+ transition is determined to be 7.0 D in the region of 3.73 Å<
R<
4.98 Å. Transition lines to the (1)3Σ+ state from the B1Π(v′=8,J′ = 15) level, which is perturbed by the (1)3Π1(v0,N=J=15) level, are measured by the Doppler-free OODRPS. The energy spacing between the F1 and F3 components of the (1)3Σ+(v=4,N=15) level is observed to be smaller than 0.001 cm-1. The hyperfine splittings, which are described by Hund's case (bβS), are observed, and the hyperfine constants ANa and ARb of the (1)3Σ+(v=4) level are determined to be 0.0293 and 0.0336 cm-1, respectively. The hyperfine splittings are identified as originating from the Fermi contact interaction. From the analysis, it is concluded that the electron spins in the (1)3Σ+ state are almost equally populated to the 5SRb and 3sNa orbitals. © 1996 American Institute of Physics.
R<
4.98 Å. Transition lines to the (1)3Σ+ state from the B1Π(v′=8,J′ = 15) level, which is perturbed by the (1)3Π1(v0,N=J=15) level, are measured by the Doppler-free OODRPS. The energy spacing between the F1 and F3 components of the (1)3Σ+(v=4,N=15) level is observed to be smaller than 0.001 cm-1. The hyperfine splittings, which are described by Hund's case (bβS), are observed, and the hyperfine constants ANa and ARb of the (1)3Σ+(v=4) level are determined to be 0.0293 and 0.0336 cm-1, respectively. The hyperfine splittings are identified as originating from the Fermi contact interaction. From the analysis, it is concluded that the electron spins in the (1)3Σ+ state are almost equally populated to the 5SRb and 3sNa orbitals. © 1996 American Institute of Physics.
- リンク情報
- ID情報
-
- DOI : 10.1063/1.472000
- ISSN : 0021-9606
- SCOPUS ID : 0030195602