> Conical intersection or curve‐crossing is well known to be an efficient dynamic funnel for nonadiabatic transition between two d'/> Nonadiabatic decay dynamics of phthalide from the light‐absorbing S <sub xmlns='http://www.wiley.com/namespaces/wiley'>3</sub>3 (ππ*) state‐resonance Raman spectroscopy and CASSCF study
首页> 外文期刊>Journal of Raman Spectroscopy: An International Journal for Original Work in All Aspects of Raman Spectroscopy, Including Higher Order Processes, and Also Brillouin- and Rayleigh Scattering >Nonadiabatic decay dynamics of phthalide from the light‐absorbing S 33 (ππ*) state‐resonance Raman spectroscopy and CASSCF study
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Nonadiabatic decay dynamics of phthalide from the light‐absorbing S 33 (ππ*) state‐resonance Raman spectroscopy and CASSCF study

机译:来自光吸收S 3 3(ππ*)状态谐振拉曼光谱和烧查的衰减动力学

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> Conical intersection or curve‐crossing is well known to be an efficient dynamic funnel for nonadiabatic transition between two different potential energy surfaces in chemical dynamics. Tremendous efforts have been made in the direct experimental probing of conical intersection. However, the direct following‐up of the dynamic process initiated from the Franck–Condon (FC) region toward a curve‐crossing point is still challenging. With the aid of complete active space self‐consistent field calculations, the resonance Raman spectroscopy has been applied to face challenges. Herein, the nonadiabatic decay dynamics of phthalide initiated from the light‐absorbing S 3 (ππ*) state were studied. The UV and vibrational spectra were assigned with the aid of the density functional theory calculations and normal‐mode analysis. The minima of the six lowest electronic excited states (S 1 , S 2 , S 3 , T 1 , T 2 , and T 3 ) and the corresponding minimum‐energy intersections were fully optimized at the complete active space self‐consistent field level. The B‐band resonance Raman spectra in acetonitrile were simulated by using the time‐dependent wave‐packet theory in a simple model to obtain the dimensionless normal‐mode displacements, and the results were compared with the relative changes of the geometric structural parameters between the curve‐crossing points and S 0 so as to help determine the decay channels initiated from the FC region. Two nonadiabatic decay channels were discovered, and that one of these had not been previously observed. The results provided general insights into the ultrafast decay dynamics initiated from the FC region of the light‐absorbing excited state to the nearby conical intersection or curve‐crossing points for organic molecules in solution. Copyright ? 2017 John Wiley & Sons, Ltd.
机译: >圆锥形交叉口或曲线交叉均可成为一种有效的动态漏斗,用于两种不同潜力之间的非等效转变化学动力学中的能量表面。已经在直接实验概率探索锥形交叉口方面取得了巨大努力。然而,从Franck-Condon(FC)区域向曲线交叉点开始的动态过程的直接跟进仍然具有挑战性。借助于完整的主动空间自我一致的场计算,共振拉曼光谱已经应用于面临挑战。这里,研究了从光吸收S 3 (π×)状态的邻苯二甲酸盐的非等离衰减动态。借助于密度泛函理论计算和正常模式分析,分配UV和振动光谱。六个最低电子激发态的最小值(S 1 ,s 2 ,s 3 ,t 1 , T 2 和t 3 )和相应的最小能量交叉点在完整的主动空间自我一致的场级完全优化。通过使用简单模型中的时间依赖波分组理论来模拟乙腈中的B波段共振拉曼光谱,以获得无量纲的正常模式位移,并且将结果与几何结构参数之间的相对变化进行比较曲线交叉点和S 0 以帮助确定从FC区域发起的衰减通道。发现了两个非抗衰减频道,并且以前未观察到其中之一。结果提供了一般的见解,进入从光吸收激发态的FC区域发起的超快衰减动态到溶液中有机分子的附近锥形交叉点或曲线交叉点。版权? 2017年John Wiley&amp; SONS,LTD。

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