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首页> 外文期刊>The Journal of Chemical Physics >ULTRAFAST QUANTUM DYNAMICS AND RESONANCE RAMAN SPECTROSCOPY OF PHOTOEXCITED I-2(B) IN LARGE ARGON AND XENON CLUSTERS
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ULTRAFAST QUANTUM DYNAMICS AND RESONANCE RAMAN SPECTROSCOPY OF PHOTOEXCITED I-2(B) IN LARGE ARGON AND XENON CLUSTERS

机译:氩和氙团簇中光激发的I-2(B)的超快量子动力学和共振拉曼光谱

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The early quantum dynamics following the B((3) Pi(0u)+) <-- X photoexcitation of I-2 in large rare gas clusters is studied and the resonance Raman spectrum of these systems is calculated by a novel time-dependent quantum mechanical simulation approach. The method used is the classically based separable potential (CSP) approximation, in which classical molecular dynamics simulations are used in a first step to determine an effective time-dependent separable potential for each mode, then followed by quantum wavepacket calculations using these potentials. In the simulations for I-2(Ar)(n) and I-2(Xe)(n), with n = 17, 47, all the modes are treated quantum mechanically. The Raman overtone intensities are computed from the multidimensional time-dependent wavepacket for each system, and the results are compared with experimental data on I-2 in Ar matrices and in liquid Xe. The main findings include: (i) Due to wavepacket dephasing effects the Raman spectra are determined well before the iodine atoms hit the rare gas ''wall'' at about 80 fs after photoexcitation. (ii) No recurrencies are found in the correlation functions for I-2(Ar)(n). A very weak recurrence event is found for I-2(Xe)(n). (iii) The simulations for I-2(Ar)(17) (first solvation layer) and for I-2(Ar)(47) (second solvation shell) show differences corresponding to moderate cluster size effects on the Raman spectra. (iv) It is estimated that coupling to the B '' ((1) Pi(1u)) state or to the a (1 g) state have a small effect on the Raman intensities. (v) For I-2(Ar)(47), the results are in very good quantitive agreement with I-2/Ar matrix experiments. The I-2(Xe)(n) results are in qualitative agreement with experiments on I-2 in liquid Xe. The reported calculations represent a first modeling of resonance Raman spectra by quantum dynamical simulations that include all degrees of freedom in large systems, and they demonstrate the power of the CSP method in this respect. (C) 1996 American Institute of Physics. [References: 58]
机译:研究了稀有气体簇中I-2的B((3)Pi(0u)+)<-X光激发后的早期量子动力学,并通过新型时变量子计算了这些系统的共振拉曼光谱机械仿真方法。所使用的方法是基于经典的可分离势(CSP)近似,其中第一步中使用经典的分子动力学模拟来确定每种模式的有效时变可分离势,然后使用这些势进行量子波包计算。在I-2(Ar)(n)和I-2(Xe)(n)的模拟中,当n = 17、47时,所有模式都被量子力学处理。从每个系统的多维时变波包计算拉曼泛音强度,并将结果与​​Ar矩阵和液体Xe中I-2的实验数据进行比较。主要发现包括:(i)由于波包的相移效应,在光激发后约80 fs碘原子撞击稀有气体“壁”之前就已经确定了拉曼光谱。 (ii)在I-2(Ar)(n)的相关函数中未发现重复发生。发现I-2(Xe)(n)的复发事件非常微弱。 (iii)对I-2(Ar)(17)(第一溶剂化层)和I-2(Ar)(47)(第二溶剂化壳)的模拟显示出与拉曼光谱上中等簇尺寸效应相对应的差异。 (iv)据估计,耦合至B”((1)Pi(1u))态或耦合至a(1 g)态对拉曼强度影响很小。 (v)对于I-2(Ar)(47),结果与I-2 / Ar矩阵实验非常吻合。 I-2(Xe)(n)结果与液体Xe中I-2的实验定性一致。所报告的计算代表了通过量子动力学模拟对共振拉曼光谱进行的第一个建模,该模拟包括大型系统中的所有自由度,并且它们在这方面证明了CSP方法的强大功能。 (C)1996年美国物理研究所。 [参考:58]

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