Pure rotational spectrum of CaCH3(X̃ 2A1) using the pump/probe microwave-optical double resonance (PPMODR) technique

1999 ◽  
Vol 110 (23) ◽  
pp. 11309-11314 ◽  
Author(s):  
Kei-ichi C. Namiki ◽  
Timothy C. Steimle
1986 ◽  
Vol 84 (3) ◽  
pp. 1317-1324 ◽  
Author(s):  
Kojiro Takagi ◽  
Shuji Saito ◽  
Tetsuo Suzuki ◽  
Eizi Hirota

1980 ◽  
Vol 73 (6) ◽  
pp. 2570-2574 ◽  
Author(s):  
Kojiro Takagi ◽  
Shuji Saito ◽  
Masao Kakimoto ◽  
Eizi Hirota

1991 ◽  
Vol 30 (36) ◽  
pp. 5270 ◽  
Author(s):  
Giorgio Zizak ◽  
Giuseppe A. Petrucci ◽  
Christopher L Stevenson ◽  
James D. Winefordner

1993 ◽  
Vol 98 (3) ◽  
pp. 1837-1842 ◽  
Author(s):  
D. A. Fletcher ◽  
K. Y. Jung ◽  
C. T. Scurlock ◽  
T. C. Steimle

1988 ◽  
Vol 66 (8) ◽  
pp. 1824-1831 ◽  
Author(s):  
Takashi Ishiwata ◽  
Osamu Nakamura ◽  
Kinichi Obi ◽  
Ikuzo Tanaka

The technique of optical–optical double resonance has been applied to a study of the [Formula: see text] ion-pair state of Br2. Two pulsed dye lasers excite the molecules from the ground state to the [Formula: see text] ion-pair state stepwise through the [Formula: see text] state in the pump-probe scheme: [Formula: see text]. The [Formula: see text] emission identified at around 215 nm is used to detect the double resonance signals when the probe laser frequency (ν2) is scanned by fixing the pump laser frequency (v1) to appropriate [Formula: see text] transitions. The emission spectra are resolved to establish the absolute vibrational numbering of the ion-pair state in terms of the Franck–Condon calculations. The Dunham coefficients of the [Formula: see text] state obtained in a global least-squares fit analysis of 377 transitions [Formula: see text] are Y00 = 57929.724(24), Y10 = 212.227(23), Y20 = −1.5683(56), Y30 = 1.606(40) × 10−2, Y01 = 0.0465652(89), Y11 = −4.500(36) × 10−4, Y21 = 1.133(41) × 10−5, and Y02 = −9.37(94) × 10−9 for 79Br2 isotope species (all in cm−1 with 3σ in parentheses).


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