Subsequenttoe\cmn\_e1.~ b>--nCO 1 laser pulse,U~oiesccnceh~beenderccted,rom 1v3 ofCHpF trappedm raregas mxrlces. Zu3 IS acavated by V-V energy transfer and deactivates at twce the rate of YJ rehntlon X kmetlc model IS presented to interpret these observations
Vibrational energy relaxation of CH3F dissolved in liquid O2 and Ar
โ Scribed by S.R.J. Brueck; T.F. Deutsch; R.M. Osgood Jr.
- Publisher
- Elsevier Science
- Year
- 1977
- Tongue
- English
- Weight
- 553 KB
- Volume
- 51
- Category
- Article
- ISSN
- 0009-2614
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โฆ Synopsis
Infrared double resonance and saturation techniques have both been used to measure the V-T relaxation of the 19 mode of CH3F in dilute solution in the cryogenic liquid hosts 02 and Ar. With the former technique, a relaxation time of 375 + 35 ns is found in liquid 02 while in liquid Ar the relaxation time is 1.30 2 0.15 c(s_ An induced v3 + 2~~ absorption is observed in the double resonance measurement; the measured anharmonicity is in good agreement with the gas phase literature value.
๐ SIMILAR VOLUMES
The energy rekstion of the lowest vibrational Ieke (U = 1) of liquid oxygen in the electronic ground state aas investigated \Cthin a wide temperature range (53.4 Ii < T < 96 R). The relaation time exhibits a peak vlllue of; = 3.1 ms around 65 I< and is shorter at loxcer and higher temperatures. The
A two-laser (IR overtone pump and UV laser-induced fluorescence probe) technique has been used to measure vibrational relaxation for NO(X \*II, v= 3) colliding with NO, 02, and CH4 at 295 K. The total removal rate coefficients are: (3.26 k 0.24) X 10-'2cm3s-'forNO,(1.46f0.15)~10-'3cm3s-'for02,and(1.