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基于含时电流密度泛函理论的π共轭低聚物的激发能

Excitation energies of pi-conjugated oligomers within time-dependent current-density-functional theory.

作者信息

van Faassen M, de Boeij P L

机构信息

Theoretical Chemistry, Materials Science Centre, Rijksuniversiteit Groningen, Nijenborgh 4, 9747 AG Groningen, The Netherlands.

出版信息

J Chem Phys. 2004 Dec 1;121(21):10707-14. doi: 10.1063/1.1810137.

Abstract

We study the pi*<--pi singlet excitations of the pi-conjugated oligomers of polyacetylene, polydiacetylene, polybutatriene, polythiophene, poly(para-phenylene vinylene), and the lowest singlet excitations of the hydrogen chain. For this we used time-dependent current-density-functional theory within the Vignale-Kohn and adiabatic local density approximations. By studying the dependence of the excitation spectrum on the chain length we conclude that the reduction of the static polarizability when using the Vignale-Kohn functional has two origins. First, the excitation energies of transitions with a large transition dipole are shifted upward. Second, the character of the transition between the lowest occupied and highest unoccupied molecular orbitals and the oscillator strength of the lowest transition within the adiabatic local density approximation is transferred to higher transitions. The lowest transitions that have a considerable oscillator strength obtained with the Vignale-Kohn functional have excitation energies that are in most cases in better agreement with available reference data than the adiabatic local density approximation.

摘要

我们研究了聚乙炔、聚二乙炔、聚丁三烯、聚噻吩、聚(对亚苯基亚乙烯基)等π共轭低聚物的π*←π单重激发以及氢链的最低单重激发。为此,我们在Vignale-Kohn和绝热局域密度近似下使用了含时电流密度泛函理论。通过研究激发光谱对链长的依赖性,我们得出结论:使用Vignale-Kohn泛函时静态极化率的降低有两个原因。首先,具有大跃迁偶极矩的跃迁的激发能向上移动。其次,最低占据分子轨道和最高未占据分子轨道之间跃迁的性质以及绝热局域密度近似下最低跃迁的振子强度转移到了更高的跃迁上。用Vignale-Kohn泛函得到的具有相当振子强度的最低跃迁的激发能,在大多数情况下比绝热局域密度近似与现有参考数据的吻合度更好。

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