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Pump-probe measurements of state-to-state rotational energy transfer rates in N2(υ = 1)

We report direct measurements of the state-to-state rotational energy transfer rates for N2 (υ=1) at 298 K. Stimulated Raman pumping of Q-branch (υ=1←0) transitions is used to prepare a selected rotational state of N2 in the υ=1 state. After allowing an appropriate time interval for collisions to oc...

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Bibliographic Details
Published in:The Journal of chemical physics 1990-12, Vol.93 (11), p.7883-7893
Main Authors: SITZ, G. O, FARROW, R. L
Format: Article
Language:English
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Summary:We report direct measurements of the state-to-state rotational energy transfer rates for N2 (υ=1) at 298 K. Stimulated Raman pumping of Q-branch (υ=1←0) transitions is used to prepare a selected rotational state of N2 in the υ=1 state. After allowing an appropriate time interval for collisions to occur, 2+2 resonance-enhanced multiphoton ionization is used (through the a 1Πg←X 1Σ+g transition) to detect the relative population of the pumped level and other levels to which rotational energy transfer has occurred. We have performed a series of measurements in which a single even rotational level (Ji=0–14) is excited and the time-dependent level populations are recorded at three or more delay times. This data set is then globally fit to determine the best set of state-to-state rate constants. The fitting procedure does not place any constraints (such as an exponential gap law) on the J or energy dependence of the rates. We compare our measurements and best-fit rates with results predicted from phenomenological rate models and from a semiclassical scattering calculation of Koszykowski et al. [J. Phys. Chem. 91, 41 (1987)]. Excellent agreement is obtained with two of the models and with the scattering calculation. We also test the validity of the energy-corrected sudden (ECS) scaling theory for N2 by using our experimental transfer rates as basis rates (J=L→0), finding that the ECS scaling expressions accurately predict the remaining rates.
ISSN:0021-9606
1089-7690
DOI:10.1063/1.459370