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气相CS二聚体的激光诱导取向动力学

Laser-induced alignment dynamics of gas phase CS dimers.

作者信息

Chatterley Adam S, Baatrup Mia O, Schouder Constant A, Stapelfeldt Henrik

机构信息

Department of Chemistry, Aarhus University, 8000 Aarhus C, Denmark.

Department of Physics and Astronomy, Aarhus University, 8000 Aarhus C, Denmark.

出版信息

Phys Chem Chem Phys. 2020 Feb 14;22(6):3245-3253. doi: 10.1039/c9cp06260b. Epub 2020 Jan 29.

Abstract

Rotational dynamics of gas phase carbon disulfide (CS) dimers were induced by a moderately intense, circularly polarized alignment laser pulse and measured as a function of time by Coulomb explosion imaging with an intense fs probe pulse. For the alignment pulse, two different temporal intensity profiles were used: a truncated pulse with a 150 ps turn-on and a 8 ps turn-off, or a 'kick' pulse with a duration of 1.3 ps. For both types of pulse, rich rotational dynamics with characteristic full and fractional revivals were recorded, showing that the intermolecular carbon-carbon axis periodically aligns along the propagation direction of the laser pulses. The truncated pulse gave the strongest alignment, which we rationalize as being due to a flat relative phase between the components in the rotational wave packet generated. Fourier analysis of the alignment dynamics gave well-spaced peaks which were fit to determine the rotational constant, B, and the centrifugal constant, D, for the ground state of the dimer. Our results agree with values from high-resolution IR spectroscopy. Numerical simulations of the alignment accurately reproduced the experimental dynamics when the truncated pulse or a low intensity kick pulse was used, but failed to reproduce the dynamics induced by a high intensity kick pulse. We posit that the discrepancy is due to excitation of the intermolecular torsional motion by the kick pulse.

摘要

气相二硫化碳(CS)二聚体的旋转动力学由中等强度的圆偏振排列激光脉冲诱导产生,并通过使用强飞秒探测脉冲的库仑爆炸成像技术作为时间的函数进行测量。对于排列脉冲,使用了两种不同的时间强度分布:一种是开启时间为150 ps、关闭时间为8 ps的截断脉冲,另一种是持续时间为1.3 ps的“踢”脉冲。对于这两种类型的脉冲,都记录到了具有特征性的全周期和分数周期复苏的丰富旋转动力学,表明分子间的碳 - 碳轴沿着激光脉冲的传播方向周期性地排列。截断脉冲产生了最强的排列,我们将其解释为是由于所产生的旋转波包中各分量之间相对相位平坦所致。对排列动力学的傅里叶分析给出了间隔良好的峰值,通过拟合这些峰值来确定二聚体基态的转动常数B和离心常数D。我们的结果与高分辨率红外光谱得到的值一致。当使用截断脉冲或低强度踢脉冲时,排列的数值模拟准确地再现了实验动力学,但未能再现由高强度踢脉冲诱导的动力学。我们认为这种差异是由于踢脉冲激发了分子间的扭转运动。

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