Intramolecular vibrational energy redistribution and conformational isomerization in vibrationally excited 2-fluoroethanol: High-resolution, microwave-infrared double-resonance spectroscopy investigation of the asymmetric –CH2(F) stretch near 2980 cm−1

1999 ◽  
Vol 110 (4) ◽  
pp. 1979-1989 ◽  
Author(s):  
David Green ◽  
Sarah Hammond ◽  
John Keske ◽  
Brooks H. Pate
1993 ◽  
Vol 99 (8) ◽  
pp. 5701-5711 ◽  
Author(s):  
Marcel Drabbels ◽  
Johannes Heinze ◽  
J. J. ter Meulen ◽  
W. Leo Meerts

1991 ◽  
Vol 11 (3-4) ◽  
pp. 237-245 ◽  
Author(s):  
Kevin K. Lehmann ◽  
Brooks H. Pate ◽  
G. Scoles

Using frequency resolved techniques we have been able to measure the rate of intramolecular vibrational energy redistribution in a number of substituted acetylenes. The method of IVR rate determination is discussed with respect to time domain measurements. The lifetimes we have determined have been quite long, ranging from a few hundred ps to a few ns. Interesting behavior of the rate as a function of the structure of the molecule has been observed. Results show sensitivity of the IVR rate to heavy mass substitution and the possibility of chromophore determined lifetimes.


1979 ◽  
Vol 57 (4) ◽  
pp. 593-600 ◽  
Author(s):  
R. H. Kagann ◽  
I. Ozier ◽  
G. A. McRae ◽  
M. C. L. Gerry

Ten pure rotational Q-branch transitions of the distortion moment spectrum of GeH4 have been measured between 9 and 23 GHz. They were observed in a conventional Stark modulated spectrometer modified to have a sensitivity of 1 × 10−11 cm−1. No Ge isotope splitting was observed in the spectrum. The spectrum was analysed in terms of a single set of six tensor centrifugal distortion constants DT, H4T, H6T, L4T, L6T, and L8T. The results were found to predict accurately transitions previously reported from infrared–microwave double resonance spectroscopy, and a complete analysis using both sets of data was carried out. The results are (in hertz): DT = 67 775.54 ± 0.86; H4T = −5.3827 ± 0.0055; H6T = 2.9693 ± 0.0019; L4T = (3.996 ± 0.088) × 10−4; L6T = −(4.122 ± 0.050) × 10−4; L8T = −(8.01 ± 0.14) × 10−4. The errors here are the standard deviations obtained from the least-squares analysis; estimates of the absolute errors are also given. For possible application in other high resolution studies, the constants have been used to calculate all tensor splittings for J ≤ 20.


1981 ◽  
Vol 6 (2) ◽  
pp. 93 ◽  
Author(s):  
Chris W. Patterson ◽  
Peter F. Moulton ◽  
A. Mooradian ◽  
Robin S. McDowell

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