首页> 外文期刊>The Journal of Chemical Physics >A MOLECULAR DYNAMICS ANALYSIS OF RESONANCE EMISSION - OPTICAL DEPHASING AND INHOMOGENEOUS BROADENING OF CH3I IN CH4 AND AR
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A MOLECULAR DYNAMICS ANALYSIS OF RESONANCE EMISSION - OPTICAL DEPHASING AND INHOMOGENEOUS BROADENING OF CH3I IN CH4 AND AR

机译:CH4和AR中CH3I的共振发射-光学脱色和非均相扩散的分子动力学分析。

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The spontaneous resonance emission of CH3I in high pressures (800-1600 psi) of CH4 and Ar excited in the region of the Rydberg B-state origin (similar to 201 nm) are reported. These emission spectra consist of narrow Raman-Like (RL) and broad fluorescence-like (FL) spectral features. The observed ratio of the Raman/fluorescence intensity in these high pressure solutions is a function of the excitation wavelength as the incident radiation is tuned through the pressure broadened electronic origin band. Molecular dynamics simulations are implemented for the analysis of the observed emission spectral shapes acid their excitation frequency dependence. The four-time dipole correlation functions required for the calculation of this nonlinear polarization derived signal are successfully approximated by a product of two two-time dipole correlation functions for these chromophore-bath systems (factorization approximation). The complex emission band shapes and their excitation frequency dependence are captured by this approach. The dispersion in the RL/FL emission redistribution is due to the multiple time scales inherent to the decay of the resonant optical coherence of these pressure-broadened absorptions. The wavelength dependent pure-dephasing rate is determined by the nonlinear shape of the solute-solvent difference potential. The observational time scale dependence of the spectroscopic homogeneous and inhomogeneous line broadening labels is clearly demonstrated and contrasted here for absorption and Raman scattering. (C) 1996 American Institute of Physics. [References: 50]
机译:据报道,在里德堡B态起源(类似于201 nm)区域激发的CH4和Ar的高压(800-1600 psi)下,CH3I的自发共振发射。这些发射光谱由窄拉曼样(RL)和宽荧光样(FL)光谱特征组成。在这些高压溶液中观察到的拉曼/荧光强度比率是激发波长的函数,因为入射辐射是通过压力加宽的电子原带进行调谐的。实施了分子动力学模拟,以分析观察到的其激发频率依赖性的发射光谱形状。对于这些生色团-浴系统,通过两个两次偶极子相关函数的乘积可以成功地近似计算此非线性偏振派生信号所需的四次偶极子相关函数(因式近似)。这种方法可以捕获复杂的发射带形状及其激励频率依赖性。 RL / FL发射重新分布中的色散是由于这些压力扩展吸收的共振光学相干性衰减所固有的多个时间尺度所致。波长相关的纯相移速率由溶质-溶剂差异电位的非线性形状确定。光谱的均匀和不均匀谱线加宽标记物在时间尺度上的依存性在这里被清楚地证明和对比,用于吸收和拉曼散射。 (C)1996年美国物理研究所。 [参考:50]

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