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Rotationally inelastic scattering of NO(A(2)Sigma(+)) + Ar: Differential cross sections and rotational angular momentum polarization

机译:NO(A(2)Sigma(+))+ Ar的旋转非弹性散射:微分截面和旋转角动量极化

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We present the implementation of a new crossed-molecular beam, velocity-map ion-imaging apparatus, optimized for collisions of electronically excited molecules. We have applied this apparatus to rotational energy transfer in NO(A(2)Sigma(+), v = 0, N = 0, j = 0.5) + Ar collisions, at an average energy of 525 cm(-1). We report differential cross sections for scattering into NO(A(2)Sigma(+), v = 0, N' = 3,5,6,7,8, and 9), together with quantum scattering calculations of the differential cross sections and angle dependent rotational alignment. The differential cross sections show dramatic forward scattered peaks, together with oscillatory behavior at larger scattering angles, while the rotational alignment moments are also found to oscillate as a function of scattering angle. In general, the quantum scattering calculations are found to agree well with experiment, reproducing the forward scattering and oscillatory behavior at larger scattering angles. Analysis of the quantum scattering calculations as a function of total rotational angular momentum indicates that the forward scattering peak originates from the attractive minimum in the potential energy surface at the N-end of the NO. Deviations in the quantum scattering predictions from the experimental results, for scattering at angles greater than 10 degrees, are observed to be more significant for scattering to odd final N'. We suggest that this represents inaccuracies in the potential energy surface, and in particular in its representation of the difference between the N- and O-ends of the molecule, as given by the odd-order Legendre moments of the surface. (C) 2015 AIP Publishing LLC.
机译:我们介绍了一种新的跨分子束,速度图离子成像仪的实现,该器件针对电子激发分子的碰撞进行了优化。我们已将此设备应用于NO(A(2)Sigma(+),v = 0,N = 0,j = 0.5)+ Ar碰撞中的旋转能量转移,平均能量为525 cm(-1)。我们报告了散射为NO(A(2)Sigma(+),v = 0,N'= 3,5,6,7,8和9)的差分截面,以及差分截面的量子散射计算和取决于角度的旋转对准。微分横截面显示出剧烈的前向散射峰,以及在较大散射角处的振荡行为,同时还发现旋转对准力矩随散射角而振荡。通常,发现量子散射计算与实验非常吻合,在较大的散射角处再现了正向散射和振荡行为。对作为总旋转角动量的函数的量子散射计算的分析表明,前向散射峰源自NO的N端势能面中的吸引极小值。对于大于10度角的散射,实验结果的量子散射预测偏差被观察到对于最终奇数N'的散射更为显着。我们建议这代表了势能表面的不精确性,特别是代表了分子的N端和O端之间的差异,这是由表面的奇数勒让德矩所给出的。 (C)2015 AIP Publishing LLC。

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