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首页> 外文期刊>The Journal of Chemical Physics >S_1-S_2 vibronic coupling in cis-1,3,5-hexatriene.II.Theoretical investigation of absorption and resonance Raman spectra
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S_1-S_2 vibronic coupling in cis-1,3,5-hexatriene.II.Theoretical investigation of absorption and resonance Raman spectra

机译:顺式1,3,5-己三烯中的S_1-S_2振动耦合.II。吸收和共振拉曼光谱的理论研究

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A wave packet prepared on the 1 ~1B_1 potential-energy surface of cis-1,3,5-hexatriene (CHT) is characterized by a very short lifetime of ≈20 fs in this state. We present here model calculations of the excited-state dynamics of CHT that are consistent with the experimentally determined population decay time scale and yield an accurate description of the absorption, preresonance and resonance Raman (RR) spectroscopy of the 1 ~1B_1 state. The greater diffuseness and complexity of the free jet 1 ~1B~1 absorption band of CHT as compared to the 1~1A_g->1 ~1B_u transition of trans-1,3,5-hexatriene can be explained by a faster optical dephasing rate and more densely spaced vibronic level structure in the S_2 state of the cis isomer primarily due to the presence of two very active low-frequency S_1-S_2 coupling modes, v_(30) and v_(31). The first measurement of the one-photon 1 ~1A_1->1 ~1A_1 transition of CHT has been reported only ten years ago and the S_1 state has since been thoroughly studied by different techniques. The simulations of the excitation and RR emission profiles of the 2 ~1A_1 state performed for this work are shown to be in quantitative agreement with the observed spectra. One of the most important and controversial questions arising from the spectroscopic information about the 1 ~1A_1 state concerns the nature of the intensity carrier for the one-photon S_0->S_1 excitation process. It can be shown that the oscillator strength for one-photon transitions into the 2 ~1A_1 vibronic manifold is exclusively borrowed from the electronic 1 ~1B_1 configuration. One model Hamiltonian is defined for the representation of wave pakcet motion in the 1 ~1A_1,2 ~1A_1, and 1 ~1B_1 states and the nuclear coordinate space comprises eight dimensions. The relevant normal modes are either of a_1 or b_1 symmetry, i.e., only first-order intrastate or S_1-S_2 vibronic coupling effects are considered,and have been selected based on the electronic structure information compiled in the preceding paper.
机译:在顺式1,3,5-己三烯(CHT)的1〜1B_1势能表面上制备的波包的特征在于,在这种状态下的寿命非常短,约为20 fs。我们在此介绍CHT激发态动力学的模型计算,该模型计算与实验确定的种群衰减时间尺度一致,并给出1〜1B_1状态的吸收,预共振和共振拉曼(RR)光谱的准确描述。与反式1,3,5-己三烯的1〜1A_g-> 1〜1B_u跃迁相比,CHT的自由射流1〜1B〜1吸收带具有更大的扩散性和复杂性,这可以用较快的光学移相速率来解释且由于两个非常活跃的低频S_1-S_2耦合模式v_(30)和v_(31)的存在,顺式异构体的S_2状态的振动能级结构更密集。 CHT的单光子1〜1A_1-> 1〜1A_1跃迁的首次测量仅在十年前才报道,此后通过不同技术对S_1状态进行了深入研究。这项工作进行的2〜1A_1状态的激发和RR发射曲线的仿真显示与观察到的光谱在数量上是一致的。关于1〜1A_1状态的光谱信息引起的最重要和最有争议的问题之一是关于单光子S_0-> S_1激发过程的强度载体的性质。可以看出,单光子跃迁到2〜1A_1振动电子歧管中的振荡器强度完全是从电子1〜1B_1配置中借用的。定义了一种哈密顿量模型,用于表示1〜1A_1,2〜1A_1和1〜1B_1状态下的波包运动,核坐标空间包括八个维度。相关的法线模式为a_1或b_1对称,即仅考虑一阶内部状态或S_1-S_2振动耦合效应,并且已根据前一论文中汇编的电子结构信息进行了选择。

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