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线性多烯低激发态的能量

Energies of low-lying excited states of linear polyenes.

作者信息

Christensen Ronald L, Galinato Mary Grace I, Chu Emily F, Howard Jason N, Broene Richard D, Frank Harry A

机构信息

Department of Chemistry, Bowdoin College, Brunswick, Maine 04011-8466, USA.

出版信息

J Phys Chem A. 2008 Dec 11;112(49):12629-36. doi: 10.1021/jp8060202.

Abstract

Room temperature absorption and emission spectra of the all-trans isomers of decatetraene, dodecapentaene, tetradecahexaene, and hexadecaheptaene have been obtained in a series of nonpolar solvents. The resolved vibronic features in the optical spectra of these model systems allow the accurate determination of S(0) (1(1)A(g)(-)) --> S(2) (1(1)B(u)(+)) and S(1) (2(1)A(g)(-)) --> S(0) (1(1)A(g)(-)) electronic origins as a function of solvent polarizability. These data can be extrapolated to predict the transition energies in the absence of solvent perturbations. The effects of the terminal methyl substituents on the transition energies also can be estimated. Franck-Condon maxima in the absorption and emission spectra were used to estimate differences between S(0) (1(1)A(g)(-)) --> S(1) (2(1)A(g)(-)) and S(0) (1(1)A(g)(-)) --> S(2) (1(1)B(u)(+)) electronic origins and "vertical" transition energies. Experimental estimates of the vertical transition energies of unsubstituted, all-trans polyenes in vacuum as a function of conjugation length are compared with long-standing multireference configuration interaction (MRCI) treatments and with more recent ab initio calculations of the energies of the 2(1)A(g)(-) (S(1)) and 1(1)B(u)(+) (S(2)) states.

摘要

已在一系列非极性溶剂中获得了癸四烯、十二碳五烯、十四碳六烯和十六碳七烯的全反式异构体的室温吸收光谱和发射光谱。这些模型体系的光谱中分辨出的振动电子特征使得能够准确测定作为溶剂极化率函数的S(0) (1(1)A(g)(-)) → S(2) (1(1)B(u)(+))和S(1) (2(1)A(g)(-)) → S(0) (1(1)A(g)(-))电子起源。这些数据可以外推以预测在无溶剂扰动情况下的跃迁能量。还可以估计末端甲基取代基对跃迁能量的影响。吸收光谱和发射光谱中的弗兰克-康登最大值用于估计S(0) (1(1)A(g)(-)) → S(1) (2(1)A(g)(-))和S(0) (1(1)A(g)(-)) → S(2) (1(1)B(u)(+))电子起源与“垂直”跃迁能量之间的差异。将未取代的全反式多烯在真空中的垂直跃迁能量作为共轭长度函数的实验估计值与长期的多参考组态相互作用(MRCI)处理以及最近对2(1)A(g)(-)(S(1))和1(1)B(u)(+)(S(2))态能量的从头算计算进行了比较。

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