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利用飞秒时间分辨光电子能谱研究斯塔克辅助的相干CS(2) 4f和5p里德堡波包的布居控制。

Stark-assisted population control of coherent CS(2) 4f and 5p Rydberg wave packets studied by femtosecond time-resolved photoelectron spectroscopy.

作者信息

Knappenberger Kenneth L, Lerch Eliza-Beth W, Wen Patrick, Leone Stephen R

机构信息

Department of Chemistry, University of California, Berkeley, California 94720, USA.

出版信息

J Chem Phys. 2007 Sep 28;127(12):124318. doi: 10.1063/1.2771165.

Abstract

A two-color (3+1(')) pump-probe scheme is employed to investigate Rydberg wave packet dynamics in carbon disulfide (CS(2) (*)). The state superpositions are created within the 4f and 5p Rydberg manifolds by three photons of the 400 nm pump pulse, and their temporal evolution is monitored with femtosecond time-resolved photoelectron spectroscopy using an 800 nm ionizing probe pulse. The coherent behavior of the non-stationary superpositions are observed through wavepacket revivals upon ionization to either the upper (12) or lower (32) spin-orbit components of CS(2) (+). The results show clearly that the composition of the wavepacket can be efficiently controlled by the power density of the excitation pulse over a range from 500 GWcm(2) to 10 TWcm(2). The results are consistent with the anticipated ac-Stark shift for 400 nm light and demonstrate an effective method for population control in molecular systems. Moreover, it is shown that Rydberg wavepackets can be formed in CS(2) with excitation power densities up to 10 TWcm(2) without significant fragmentation. The exponential 1e population decay (T(1)) of specific excited Rydberg states are recovered by analysis of the coherent part of the signal. The dissociation lifetimes of these states are typically 1.5 ps. However, a region exhibiting a more rapid decay ( approximately 800 fs) is observed for states residing in the energy range of 74 450-74 550 cm(-1), suggestive of an enhanced surface crossing in this region.

摘要

采用双色(3 + 1('))泵浦 - 探测方案研究二硫化碳(CS₂(*))中的里德堡波包动力学。通过400 nm泵浦脉冲的三个光子在4f和5p里德堡流形内创建态叠加,并使用800 nm电离探测脉冲通过飞秒时间分辨光电子能谱监测它们的时间演化。通过电离到CS₂⁺的上(¹²)或下(³²)自旋 - 轨道分量时的波包复兴,观察到非定态叠加的相干行为。结果清楚地表明,在500 GW/cm²至10 TW/cm²的范围内,波包的组成可以通过激发脉冲的功率密度有效控制。结果与400 nm光预期的交流斯塔克位移一致,并证明了一种在分子系统中进行布居控制的有效方法。此外,结果表明,在激发功率密度高达10 TW/cm²的情况下,CS₂中可以形成里德堡波包而不会有明显的碎片化。通过分析信号的相干部分,恢复了特定激发里德堡态的指数型粒子数衰减(T₁)。这些态的解离寿命通常为1.5 ps。然而,对于位于74450 - 74550 cm⁻¹能量范围内的态,观察到一个衰减更快(约800 fs)的区域,这表明该区域存在增强的表面交叉。

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