An investigation of the (ν2 + ν1)−ν2 hot band of FC15N by infrared-microwave double resonance

1983 ◽  
Vol 98 (2) ◽  
pp. 498-501 ◽  
Author(s):  
John Sheridan ◽  
Harold Jones
Keyword(s):  
2015 ◽  
Vol 143 (8) ◽  
pp. 084310 ◽  
Author(s):  
P. Bryan Changala ◽  
Joshua H. Baraban ◽  
Anthony J. Merer ◽  
Robert W. Field

1994 ◽  
Vol 187 (1-2) ◽  
pp. 57-72 ◽  
Author(s):  
J. Oomens ◽  
L. Oudejans ◽  
J. Reuss ◽  
A. Fayt
Keyword(s):  

1979 ◽  
Vol 57 (3) ◽  
pp. 397-401 ◽  
Author(s):  
M. Herman ◽  
J. W. C. Johns ◽  
A. R. W. McKellar

Laser Stark spectra have been observed in the (020) ← (010) hot band of H216O. A near coincidence between the 15–14 P(11) line of the 13C18O laser at 1677.228 cm−1 and the 606 ← 515 rovibrational transition of H2O as analyzed with the result: [Formula: see text]. Using the same laser line, an infrared–radiofrequency double resonance signal arising from the 422–515 transition within the (010) vibrational state was measured to be: 2159.98 ± 0.3 MHz.


1960 ◽  
Vol 57 ◽  
pp. 926-930 ◽  
Author(s):  
Jacubowicz ◽  
J. Uebersfeld
Keyword(s):  

1974 ◽  
Vol 35 (C1) ◽  
pp. C1-67-C1-72 ◽  
Author(s):  
L. PFEIFFER
Keyword(s):  

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