Sun Zhigang, Fu Bina, Zhang Dong H, Lee Soo-Y
Division of Chemistry and Biological Chemistry, School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore 637371, Singapore.
J Chem Phys. 2009 Jan 28;130(4):044312. doi: 10.1063/1.3068709.
The femtosecond stimulated Raman scattering (FSRS) difference spectra of CDCl(3) from the ground potential energy surface, with and without off-resonance impulsive stimulated Raman pumping, taken at various delay times from the impulsive pump by Kukura et al. [Phys. Rev. Lett. 96, 238303 (2006)], showed sidebands of the C-Cl bends with periodic changes in phase as well as having an inversion symmetry to the high and low frequency sides of the Stokes C-D stretch at 2255 cm(-1). The semiclassical coupled-wave approach and a one-dimensional (1D) oscillator model for the C-D stretch whose frequency is modulated in time by the C-Cl bends could account for some features of the experimental results. Here, a quantum mechanical investigation is made of the FSRS difference spectra with a modulated 1D oscillator and three-dimensional (3D) harmonic and anharmonic potentials. It is shown that (i) the sidebands are allowed, with or without anharmonic coupling between the C-D stretch and the C-Cl bends, (ii) in the 3D harmonic model the sidebands have mirror symmetry about the Stokes C-D stretch, (iii) in the 3D anharmonic model with appropriate coupling terms between the C-D stretch and the C-Cl bends, the experimental results are well accounted for in both the phase changes in the FSRS difference spectra with time delay as well as the inversion symmetry of the sidebands for the C-Cl bends about the Stokes C-D stretch, (iv) there is a correspondence between the phase changes in the FSRS difference spectra and the wavepacket motion induced by the impulsive pump pulse on the ground potential energy surface as a function of the delay time, and (v) changing the polarization of the impulsive pump pulse, say, directly affects the coordinate dependence of the linear transition dipole moment in the asymmetric mode and hence its phase in the FSRS difference spectra, but not so for the symmetric modes where the displacement of the excited state surface governs the FSRS difference spectra more than the transition dipole moment. This work illustrates the potential of off-resonance FSRS in studying polyatomic molecular dynamics.
久库拉等人[《物理评论快报》96, 238303 (2006)]在从脉冲泵浦开始的不同延迟时间下,获取了处于基态势能面的CDCl₃的飞秒受激拉曼散射(FSRS)差谱,有和没有非共振脉冲受激拉曼泵浦的情况。这些差谱显示了C-Cl弯曲的边带,其相位有周期性变化,并且对于2255 cm⁻¹处斯托克斯C-D伸缩的高频和低频侧具有反演对称性。C-D伸缩的频率由C-Cl弯曲随时间调制的半经典耦合波方法和一维(1D)振子模型可以解释实验结果的一些特征。在此,对具有调制的1D振子以及三维(3D)谐振和非谐振势的FSRS差谱进行了量子力学研究。结果表明:(i) 无论C-D伸缩和C-Cl弯曲之间有无非谐耦合,边带都是允许的;(ii) 在3D谐振模型中,边带关于斯托克斯C-D伸缩具有镜像对称性;(iii) 在C-D伸缩和C-Cl弯曲之间具有适当耦合项的3D非谐模型中,实验结果在FSRS差谱随时间延迟的相位变化以及C-Cl弯曲边带关于斯托克斯C-D伸缩的反演对称性方面都得到了很好的解释;(iv) FSRS差谱中的相位变化与脉冲泵浦脉冲在基态势能面上诱导的波包运动随延迟时间的函数关系之间存在对应关系;(v) 例如,改变脉冲泵浦脉冲的偏振直接影响不对称模式下线性跃迁偶极矩的坐标依赖性,从而影响其在FSRS差谱中的相位,但对于对称模式则不然,在对称模式中,激发态表面的位移比跃迁偶极矩对FSRS差谱的影响更大。这项工作说明了非共振FSRS在研究多原子分子动力学方面的潜力。