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传统能带图能否描述掺杂共轭聚合物的电子结构?掺杂聚3-己基噻吩的TD-DFT和自然过渡轨道研究

Does the Traditional Band Picture Describe the Electronic Structure of Doped Conjugated Polymers? TD-DFT and Natural Transition Orbital Study of Doped P3HT.

作者信息

Wu Eric C, Schwartz Benjamin J

机构信息

Department of Chemistry and Biochemistry University of California, Los Angeles, Los Angeles, California 90095-1569, United States.

出版信息

J Chem Theory Comput. 2023 Oct 10;19(19):6761-6769. doi: 10.1021/acs.jctc.3c00743. Epub 2023 Sep 28.

Abstract

Polarons and bipolarons are created when one or two electrons are removed from the π-system of a -type conjugated polymer, respectively. In the traditional band picture, the creation of a polaron causes two electronic energy levels to move into the band gap. The removal of a second electron to form a bipolaron causes the two intragap states to move further into the gap. Several groups, however, who looked at the energies of the Kohn-Sham orbitals from DFT calculations, have recently argued that the traditional band picture is incorrect for explaining the spectroscopy of doped conjugated polymers. Instead, the DFT calculations suggest that polaron creation causes only one unoccupied state to move into the band gap near the valence band edge while half-filled state in the valence band and the conduction band bend downward in energy. To understand the discrepancy, we performed TD-DFT calculations of polarons and bipolarons on poly(3-hexylthiophene) (P3HT). Not only do the TD-DFT-calculated absorption spectra match the experimental absorption spectra, but an analysis using natural transitional orbitals (NTOs), which provides an approximate one-electron picture from the many-electron TD-DFT results, supports the traditional band picture. Our TD-DFT/NTO analysis indicates that the traditional band picture also works for bipolarons, a system for which DFT calculations were unable to determine the electronic structure.

摘要

当从α型共轭聚合物的π体系中分别移除一个或两个电子时,会产生极化子和双极化子。在传统的能带图像中,极化子的产生会使两个电子能级移动到带隙中。移除第二个电子形成双极化子会使两个带隙内状态进一步移入带隙。然而,最近一些通过密度泛函理论(DFT)计算研究了Kohn-Sham轨道能量的团队认为,传统的能带图像对于解释掺杂共轭聚合物的光谱是不正确的。相反,DFT计算表明,极化子的产生只会使一个未占据状态移动到价带边缘附近的带隙中,而价带中的半填充状态和导带在能量上向下弯曲。为了理解这种差异,我们对聚(3-己基噻吩)(P3HT)上的极化子和双极化子进行了含时密度泛函理论(TD-DFT)计算。TD-DFT计算得到的吸收光谱不仅与实验吸收光谱相匹配,而且使用自然过渡轨道(NTO)进行的分析(该分析从多电子TD-DFT结果中提供了一个近似的单电子图像)支持了传统的能带图像。我们的TD-DFT/NTO分析表明,传统的能带图像也适用于双极化子,而对于双极化子体系,DFT计算无法确定其电子结构。

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