The rate of vibrational energy transfer from CHsBr&) to HCN&) has been determined to be 75 f 25 rns-' Torr-I. The factors which determine the relative importance of intermolecular vibrational energy transfer pathways will be discuswd.
Vibration-vibration energy transfer iln CH3F
β Scribed by Z. Karny; A.M. Ronn; Eric Weitz; G.W. Flynn
- Publisher
- Elsevier Science
- Year
- 1972
- Tongue
- English
- Weight
- 304 KB
- Volume
- 17
- Category
- Article
- ISSN
- 0009-2614
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β¦ Synopsis
Previous works have reported vibration-vibration
and vibration-translation transfer rates in CHJF and CHg F-X mixtures. fn this letter we report the study of the fast V-V transfer rate populating the 3~3, u1 and ~4 states of CHJF. GaseousCHsF was initially exited to the ~3 state by a TEA CO2 laser operating on the P(20) 9.6 g line and collisional pumping to the 3~3, ur and v4 states was measured by monitoring the rise time of the fluorescence at 3000 cm-'. The rate constant was found to be 2.2 X 10s set-r tom-'.
π SIMILAR VOLUMES
Infrared fluorescence from the IQ and v4 vibrational levels has been observed in CDaF following excitation by a 10.6 fi Q-switch COa laser. The exponential deactivation rate constant has been found to be 0.44 ms-r torr-t for the pure gas. The rate constants for deactivation by the rare gases have a
The rate of vibration to vibration energy transfer from CH3F excited to ~3 = 1 at 1050 cm-l to the nitric oxide and carbon monoxide fust vibrationally excited states at 1875 cm-1 and 2143 cm-t, respectively, has been measured. The V-V crossover rate was determined to be 5.5 -C 0.5 msec-r torr-' for
ti general formula of the probability of vibrational transitions in diatomic molecules is formulated with specific consideration of vibration-vibration energy transfer for nonresonant cases. An application to HZ-H2 collisions shows an excellent agreement of the present formulation with exact quantum
The vibration-vibration ene=y transfer of HCI gas initially excited to the tirst vibrational level is measured by monitoring the fluorescence of the 2-1 transition. The rate constant for the process is found to be 0.9 x IO5 secwl tom-'.