Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
5429005 | Journal of Quantitative Spectroscopy and Radiative Transfer | 2012 | 7 Pages |
The vibrational levels of KH(X1Σ+, vâ³=0-3) were generated in the reaction of K (5P) and H2. Vibrational state total relaxation rate coefficientskvâ³(CO2) for KH (vâ³=14-21) are measured in an overtone pump-probe configuration. The rate coefficient kvâ³(CO2) is strongly dependent on vibrational quantum number. Scattered CO2 (0000, 32â¤Jâ¤48) molecules were excited to CO2 (1005, J+1) states. The rotational temperatures of CO2 (0000, J=32-48) states populated by collisions with highly vibrationally excited KH (vâ³=14-21) are obtained. The average rotational energy of the scattered CO2 molecules is increased by a factor of 2.33 when KH level vâ³=14 increases to vâ³=21. The average translational energy of the scattered CO2 molecules is increased roughly linearly as a function of CO2J state. Under single collision conditions, state-specific energy transfer rate coefficients for collisions of highly excited KH with CO2 are obtained. For vâ³=19, the integrated rate coefficients kint increases by a factor of 4.5 to vâ³=14.
⺠KH (vâ³=14-21) total relaxation rate coefficients by CO2 are measured accurately. ⺠The average rotational energy of scattered CO2 increases by a factor of 2.33 when vâ³=14 to vâ³=21. ⺠The average translational energy in scattered CO2 increases linearly as a function of J state. ⺠For vâ³=19, the integrated rate coefficients KH (v) increases by a factor of 4.5 to vâ³=14.