State-Specific (Linear-Response)-Polarizable Continuum Models/Time-Dependent Density Functional Theory Study on the Absorption and Emission Spectra of an Organic Fluorescent Emitter

被引:4
作者
Liu Xiao-Jun [1 ,2 ]
Lin Tao [1 ]
Cai Xin-Chen [1 ]
Gao Shao-Wei [1 ]
Yang Lei [1 ]
Ma Rui [1 ]
Zhang Jin-Yue [1 ]
机构
[1] Beijing Jiaotong Univ, Key Lab Luminescence & Opt Informat, Minist Educ, Inst Optoelect Technol, Beijing 100044, Peoples R China
[2] Chinese Acad Sci, Key Lab Photochem Convers & Optoelect Mat, Tech Inst Phys & Chem, Beijing 100190, Peoples R China
基金
中国国家自然科学基金;
关键词
Time-dependent density functional theory; State-specific polarizable continuum model; UV-Vis spectrum; Global hybrid; Linear-response polarizable continuum model; ELECTRONIC EXCITATION-ENERGIES; LINEAR-RESPONSE METHODS; TRANSFER EXCITED-STATES; CHARGE-TRANSFER; OPTICAL-PROPERTIES; SOLVATION MODELS; BASIS-SET; MOLECULES; TDDFT; DFT/TDDFT;
D O I
10.3866/PKU.WHXB201204193
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
3-(dicyanomethylene)-5,5-dimethyl-1-(3-[9-(2-ethyl-hexyl)-carbazol]-vinyl) cyclohexene (DCDHCC) is one of a series of organic dyes with good emission performance in photoelectric devices. The absorption and emission spectra of DCDHCC were computed using PBE0O, BMK, and M06 hybrids in the frame of time-dependent density functional theory (TDDFT) in combination with polarizable continuum models (PCMs). Linear-response (LR) and state-specific (SS) PCM approaches were used as well as 6-31G(d) and 6-31+G(d,p) basis sets. The absorption and emission spectra were calculated in benzene, tetrahydrofuran, and acetone and compared with experimental observations. On the one hand, choice of hybrids was found to have a greater effect on the absorption spectra than the basis sets or the solvent model and BMK was established to be a suitable functional for the calculation of the absorption spectra of DCDHCC, on the other hand, the basis set used had a significant impact on the geometries of the excited states and thus the emission spectra, and the 6-31+G(d,p) basis set was necessary for the optimization of the excited states. It is envisaged that our calculations may be of assistance in the design of analogous emitters.
引用
收藏
页码:1329 / 1336
页数:8
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