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DFT/TDDFT 研究二苯基氮杂芴衍生物的电子结构和光谱性质。

DFT/TDDFT study on the electronic structure and spectral properties of diphenyl azafluoranthene derivative.

机构信息

Faculty of Electrical Engineering, Czȩstochowa University of Technology, Al. Armii Krajowej 17, 42-200, Czestochowa, Poland.

出版信息

J Fluoresc. 2012 Jan;22(1):81-91. doi: 10.1007/s10895-011-0932-1. Epub 2011 Aug 19.

DOI:10.1007/s10895-011-0932-1
PMID:21853258
Abstract

Paper reports the DFT/TDDFT study on the electronic structure and spectral properties of the five-membered annulated diphenyl azafluoranthene derivative 1,3-diphenyl-3H-indeno[1,2,3-de]pyrazolo[3,4-b]quinoline (DPIPQ) by means of polarizable continuum model (PCM) and Onsager reaction field approaches at the B3LYP/6-31+G(d,p) level of theory. The results of calculations are compared with the optical absorption and fluorescence spectra as well as with the cyclic voltammetry data. The DFT/TDDFT/PCM approaches exhibit rather good quantitative agreement regarding the spectral position of the first absorption band; the discrepancy between the experiment and theory is less than 0.06 eV (linear response approach) or 0.25 eV (state specific approach). As for the fluorescence emission the TDDFT/PCM calculations underestimate the transition energy on about of 0.7-0.8 eV. Such discrepancy should be attributed to insufficient quality of the TDDFT/PCM optimization in the excited state. Ignoring the geometrical relaxation in the excited state provides considerably better agreement between the experiment and theory; discrepancy is less than 0.1-0.22 eV depending on a solvent polarity. The dominant influence on the fluorescence emission results mainly from the solvent reorganization in the excited state whereas the solute relaxation is indeed weak and may be ignored.

摘要

本文采用极化连续模型(PCM)和 Onsager 反应场方法,在 B3LYP/6-31+G(d,p)理论水平上,对五员稠合二苯基氮杂芴衍生物 1,3-二苯基-3H-茚并[1,2,3-de]吡唑[3,4-b]喹啉(DPIPQ)的电子结构和光谱性质进行了密度泛函理论(DFT)/含时密度泛函理论(TDDFT)研究。计算结果与光学吸收光谱、荧光光谱和循环伏安法数据进行了比较。对于第一吸收带的光谱位置,DFT/TDDFT/PCM 方法表现出相当好的定量一致性;实验与理论之间的差异小于 0.06 eV(线性响应方法)或 0.25 eV(态特定方法)。对于荧光发射,TDDFT/PCM 计算低估了跃迁能约 0.7-0.8 eV。这种差异归因于激发态 TDDFT/PCM 优化的质量不足。在激发态中忽略几何弛豫,可以在实验和理论之间提供更好的一致性;差异小于 0.1-0.22 eV,取决于溶剂的极性。荧光发射的主要影响主要来自于激发态中的溶剂重排,而溶质弛豫确实较弱,可以忽略不计。

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