School of Engineering and Physical Sciences, Heriot-Watt University, Edinburgh, EH14 4AS, United Kingdom.
J Phys Chem A. 2009 Dec 31;113(52):15156-70. doi: 10.1021/jp905348c.
Two color polarization spectroscopy has been employed to measure the collisional depolarization of OH(A(2)Sigma(+), v = 1) by He and Ar. Complementary experiments using Zeeman quantum beat spectroscopy have also been performed to determine separately the cross sections for rotational energy transfer (RET) out of selected rotational levels of OH(A, v = 0) + Ar, as well as those for elastic depolarization. This has been achieved by dispersing the emission, so as to observe a single fluorescence transition. Elastic depolarization of OH(A) by Ar is found to be significant with that for loss of rotational alignment exceeding that for loss of orientation. In the case of OH(A) + He, the polarization spectroscopy measurements suggest that elastic depolarization plays a relatively minor role in the loss of the polarization signal compared with RET. The experimental data for OH(A) + Ar are compared in detail with the results of quasi-classical trajectory calculations that accommodate the effects of electron spin. These classical calculations are assessed against the results obtained using full close-coupled open shell quantum mechanical scattering methods. Overall the level of agreement between the two experiments, and between experiment and theory, is very reasonable. Surprisingly, at low N the elastic depolarization cross sections for OH(A) + Ar are found to be quite similar in magnitude to those observed for OH(X) + Ar despite the fact that the well depth in the latter system is considerably smaller than that for OH(A)-Ar. However, for OH(A) + Ar the depolarization cross sections are insensitive to N in the range 1-14. It is proposed that this behavior partly reflects the relatively anisotropic nature of the potential energy surface, which exhibits deep wells of different depths at the two linear configurations OH(A)-Ar and Ar-OH(A), and partly the nature of elastic depolarizing collisions, which must occur with a velocity component perpendicular to the plane of rotation of the diatomic molecule.
双色偏振光谱学已被用于测量 OH(A(2)Sigma(+), v = 1) 与 He 和 Ar 的碰撞去偏振。互补的使用塞曼量子拍频光谱学的实验也已经进行,以分别确定 OH(A, v = 0) + Ar 中选定的转动能级的转动能量转移 (RET) 的截面,以及那些用于弹性去极化的截面。这是通过分散发射来实现的,以便观察单个荧光跃迁。发现 OH(A) 与 Ar 的弹性去极化是显著的,其旋转对准的损失超过了取向的损失。在 OH(A) + He 的情况下,偏振光谱学测量表明与 RET 相比,弹性去极化在偏振信号的损失中起着相对较小的作用。OH(A) + Ar 的实验数据与准经典轨迹计算的结果进行了详细比较,该计算考虑了电子自旋的影响。这些经典计算与使用全紧密耦合开壳量子力学散射方法获得的结果进行了评估。总体而言,两个实验之间以及实验与理论之间的一致性水平非常合理。令人惊讶的是,在低 N 时,OH(A) + Ar 的弹性去极化截面的大小与观察到的 OH(X) + Ar 相当,尽管在后一个系统中阱的深度比 OH(A)-Ar 小得多。然而,对于 OH(A) + Ar,去极化截面在 1-14 的范围内对 N 不敏感。有人提出,这种行为部分反映了势能面的相对各向异性,该势能面在两个线性构型 OH(A)-Ar 和 Ar-OH(A) 处具有不同深度的深阱,部分反映了弹性去极化碰撞的性质,这种碰撞必须在与双原子分子的旋转平面垂直的速度分量下发生。