Depolarisation of rotational orientation and alignment of OH (X2Π) in collisions with molecular partners: N2 and O2

被引:16
作者
Paterson, Grant [1 ]
Marinakis, Sarandis [1 ]
Costen, Matthew L. [1 ]
McKendrick, Kenneth G. [1 ]
机构
[1] Heriot Watt Univ, Sch Engn & Phys Sci, Edinburgh EH14 4AS, Midlothian, Scotland
基金
英国工程与自然科学研究理事会;
关键词
INFRARED ACTION SPECTROSCOPY; POTENTIAL-ENERGY SURFACE; ATMOSPHERIC-PRESSURE FLAMES; PI-ELECTRONIC STATES; POLARIZATION SPECTROSCOPY; INELASTIC-COLLISIONS; QUANTUM SCATTERING; CROSS-SECTIONS; LAMBDA-DOUBLET; TEMPERATURE-DEPENDENCE;
D O I
10.1039/b909051g
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
The depolarisation of selected OH (X-2 Pi(3/2) v = 0, J = 1.5 and 4.5, e) levels in collisions with the molecular partners N-2 and O-2 at room temperature (nominally 298 K) has been studied using the polarisation spectroscopy (PS) technique. We obtain total depolarisation rate constants, k(PS)((K)), which are the combination of population transfer out of the initial level and elastic depolarisation of the tensor moment of respective rank K = 1 (orientation) or K = 2 (alignment) of its angular momentum distribution. N-2 causes more rapid decay of PS signals than O-2. There are no clear dependences of k(PS)((K)) on J for either partner. The K-dependence for N-2 mirrors that determined previously for the noble gases, but is less regular for O-2, warranting further investigation. Comparison with independent line-broadening data suggests that there may be an additional, pure-elastic-dephasing contribution to collisional broadening for N-2 that is not apparent for O-2. The presence of an independently established deeper HO-OO attractive minimum at shorter range clearly does not outweigh other factors that favour k(PS)((K)) for N-2. The most obvious explanation is stronger, longer-range attractive interactions due to the larger quadrupole moment of N-2. However, this appears to be contradicted by the rigorous ab initio calculations currently available on OH-O-2.
引用
收藏
页码:8813 / 8820
页数:8
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