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1.
以密度泛函理论结合跳跃模型, 重点研究了氯原子和烷基链的引入对吲哚并咔唑类衍生物传输性质的影响. 计算结果表明, 与吲哚并[3,2-b]咔唑(1)相比, 氯原子的引入增大了2,8-二氯吲哚并[3,2-b]咔唑(2)和2,8-二氯-5,11-二己基吲哚并[3,2-b]咔唑(3)的最高占据分子轨道(HOMO)的离域程度, 而对最低未被占据分子轨道(LUMO)则无显著贡献, 但明显降低了二者的能级. 上述结果表明, 对于LUMO, 氯原子体现了吸电子效应, 而对于HOMO, 氯原子体现了共轭效应. 烷基链的引入使化合物3的空穴迁移率明显高于化合物1和2, 这主要归因于化合物3具有更加紧密的分子堆积, 尤其在跳跃路径A中, 具有更大的分子间电子耦合和轨道重叠. 同时能带结构的计算结果进一步证明, 氯原子和烷基链的同时引入大大改善了吲哚并咔唑类衍生物的电荷传输性能.  相似文献   

2.
利用密度泛函方法(DFT)和单激发组态相互作用(CIS)方法, 在6-31G(d,p) 基组水平下优化了咔唑分子和14种双咔唑结构异构体的基态和激发态结构, 在此基础上, 用含时密度泛函(TD-DFT)方法在相同基组水平下计算了模型分子的吸收和发射波长及电荷跃迁性质. 讨论了双咔唑构型的变化带来的性质上的变化, 与实验值相比得到了精确的计算结果. 通过双咔唑的前线轨道能量值、电离能和亲和势及重组能的变化, 全面研究了不同构型的应用, 为实验上的设计和合成提供了思路.  相似文献   

3.
3-(二氰亚甲基)-5,5-二甲基-1-(3-[9-(2-乙基-己基)-咔唑基]-乙烯基)环己烷(DCDHCC)是一种用于光电器件中的有机染料,它具有良好的发光特性.我们使用含时密度泛函方法(TD-PBE0,TD-BMK和TD-M06)以及极化连续模型(PCM)计算了该材料在溶剂中的吸收和发射特性.计算中使用了线性响应(LR)、态定(SS)两种溶剂模型和6-31G(d)、6-31+G(d,p)两种基组.计算了DCDHCC在苯、四氢呋喃和丙酮溶剂中的吸收和发射光谱,并与实验观测进行了比较.结果表明:对于吸收光谱的计算,杂化函数的影响大于基组和溶剂模型,在三种函数中BMK更适于研究DCDHCC的吸收光谱;而对于发射光谱,基组的影响最大,基组通过影响激发态构型从而影响发射光谱,对于激发态构型的优化需要使用6-31+G(d,p)基组.我们希望这些研究能对今后设计类似的发光分子有帮助.  相似文献   

4.
应用密度泛函理论(DFT)和含时密度泛函理论(TDDFT)方法及连续极化模型研究了六种荧光材料分子基态和第一激发态的电子结构性质.这六种分子是:3-(二氰亚甲基)-5,5-二甲基-1-(3-[9-(2-乙基-己基)-咔唑基]-乙烯基)环己烷(DCDHCC),DCDHCC2,3-(二氰亚甲基)-5,5-二甲基-1-(4-二苯基氨基-苯乙烯基)环己烷(DCDPC),DCDPC2,3-(二氰亚甲基)-5,5-二甲基-1-(4-[9-咔唑基]-乙烯基)环己烷(DCDCC)和3-(二氰亚甲基)-5,5-二甲基-1-(4-二甲基氨基-苯乙烯基)环己烷(DCDDC).它们可作为有机发光显示器件的发光材料.比较了PBE0、M06、BMK、M062X和CAM-B3LYP五种泛函,其中BMK方法很好地再现了各个分子在丙酮溶剂中的吸收和发射光谱.同时计算了分子的电子亲和能和电离势并用于评价分子的电荷注入性质.研究表明,当使用双π桥和双受体时,分子的发射光谱会红移到理想的发光区域.据此设计了两个新的分子DCDCC2和DCDDC2,它们分别是DCDCC和DCDDC的双支对应分子.计算结果表明这两个分子也具有作为荧光发射体的良好性质.  相似文献   

5.
刘小君  王宁  程浩 《物理化学学报》2011,27(7):1640-1646
用含时密度泛函方法研究了具有推拉结构的有机发光材料3-(二氰亚甲基)-5,5-二甲基-1-(4-[9-咔唑基]-苯乙烯基)环己烯(DCDCC)的吸收和荧光光谱, 并考虑了溶剂效应. 通过与实验光谱的比较, 重点评价了包括局域和长程在内的8种交换泛函. 结果表明泛函的选择对结果的可靠性至关重要, 在密度泛函和含时密度泛函理论框架下, 包含44% Hartree Fock交换泛函的BMK杂化函数联同连续极化模型和中等大小的基组最适合研究DCDCC分子的光谱性质. 此外, 尽管DCDCC分子内电荷转移并没有强致发出双荧光, 但仍然可以用平面分子内电荷转移和扭转分子内电荷转移模型解释DCDCC激发态的结构. BMK泛函计算的结果表明DCDCC的激发态结构支持平面分子内电荷转移模型.  相似文献   

6.
用密度泛函B3LYP方法对3-(3'-吡啶基)-6-芳基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑衍生物(芳基为苯基、3-吡啶基和苯乙烯基)进行基态几何构型全优化,计算分子的电离势I_p和电子亲和势E_A等相关能量,并用Zerner间略微分重叠(ZINDO)和含时密度泛函(TDDFT)方法计算吸收光谱,用单组态相互作用方法(CIS)优化三种化合物分子的S_1激发态结构,分析其能量与发射光谱的关系,计算溶剂中分子的吸收和发射光谱,并与实验结果对照.计算结果表明,从3-(3'-吡啶基)-6-苯基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物A)到3-(3'-吡啶基)-6-(3'-吡啶基)-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物B)以及3-(3'-吡啶基)-6-对乙烯苯基-1,2,4-三唑并[3,4-b]- 1,3,4-噻二唑分子(化合物C)的电子亲和势依次增大,愈来愈容易接受电子,吸收光谱和发射光谱红移.  相似文献   

7.
李会学  唐惠安  杨声  萧泰 《物理化学学报》2007,23(11):1781-1786
用密度泛函B3LYP方法对3-(3’-吡啶基)-6-芳基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑衍生物(芳基为苯基、3-吡啶基和苯乙烯基)进行基态几何构型全优化, 计算分子的电离势IP和电子亲和势EA等相关能量, 并用Zerner间略微分重叠(ZINDO)和含时密度泛函(TDDFT)方法计算吸收光谱, 用单组态相互作用方法(CIS)优化三种化合物分子的S1激发态结构, 分析其能量与发射光谱的关系, 计算溶剂中分子的吸收和发射光谱, 并与实验结果对照. 计算结果表明, 从3-(3’-吡啶基)-6-苯基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物A)到3-(3’-吡啶基)-6-(3’-吡啶基)-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物B)以及3-(3’-吡啶基)-6-对乙烯苯基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑分子(化合物C)的电子亲和势依次增大, 愈来愈容易接受电子, 吸收光谱和发射光谱红移.  相似文献   

8.
采用密度泛函理论(DFT)和含时密度泛函理论(TD-DFT)方法计算了4种N,N-B螯合物1,1q,2和2q的基态和激发态结构、吸收和发射光谱、跃迁密度矩阵、分子内电荷转移特征、黄昆(HR)因子、FranckCondon因子和电子耦合等光物理性质,深入探究化合物1q和2q在几何结构微调后发光效率降低的本质原因.计算结果表明,N,N-B螯合物中喹啉取代吡啶,以及吲哚配体中N杂原子的引入对光物理性质产生了较大影响.相比于化合物1和2,化合物1q和2q由于共轭面的扩展导致HOMO-LUMO能隙变窄,使吸收红移.通过计算HR因子和跃迁密度矩阵对激发态的特征和几何弛豫进行分析,结果表明化合物1q和2q具有明显增强的片段间电荷转移特征,发射能和振子强度减弱导致kr减小,并且激发态和基态间的电子耦合急剧增强造成快速的非辐射衰变,导致化合物1q和2q在CH2Cl2溶液中不发光.同时,化合物1和2具有高效的发光效率和较大的斯托克斯位移,是一类有发展前景的发光材料.  相似文献   

9.
7-氮杂吲哚衍生物分子基态和激发态性质的理论研究   总被引:5,自引:0,他引:5  
用从头算HF和密度泛函B3LYP方法对7-氮杂吲哚衍生物1,3-二(N-7-氮杂吲哚基)苯、1,3,5 三(N-7-氮杂吲哚基)苯和4,4′-二(N-7-氮杂吲哚基)联苯进行全优化, 计算分子的电离势IP和电子亲和势EA等相关能量, 并用ZINDO和TDDFT方法计算吸收光谱, 用CIS优化三种化合物分子的S1激发态结构, 并分析其能量与发射光谱的关系, 计算溶剂中分子的吸收和发射光谱, 并与实验结果对照. 计算结果表明, 从7-氮杂吲哚到上述三种衍生物依次愈来愈容易接受空穴, 吸收和发射光谱红移.  相似文献   

10.
陈奔  何荣幸  李明 《物理化学学报》2010,26(9):2515-2522
苯并蒽酮衍生物在新型荧光材料、非线性光学材料和液晶显示材料等领域有较大的应用前景.本文采用量子化学方法优化了3-吡咯烷基苯并蒽酮的基态几何结构和第一单重激发态的几何结构,并与X射线晶体衍射实验值进行了对比.利用含时密度泛函理论(TD-DFT)的不同泛函,计算了3-吡咯烷基苯并蒽酮在气相和溶剂中的吸收和发射光谱,考察了它的电子结构和光谱特征,并分析了不同泛函、基组以及溶剂效应对吸收和发射光谱的影响.计算结果表明:3-吡咯烷基苯并蒽酮的最强吸收和发射光谱都是具有π→π*跃迁特征的电荷转移(CT)态;泛函B3LYP能较好地重现实验吸收能;而对于具有分子内电荷转移特征的激发态,泛函MPWK能较好地重现实验发射能.溶剂效应的计算表明,不同极性的溶剂对3-吡咯烷基苯并蒽酮的吸收光谱和发射光谱的影响较小.理论预测的光谱与实验结果一致.  相似文献   

11.
Fluoranthene and benzo[k]fluoranthene-based oligoarenes are good candidates for organic light-emitting diodes (OLEDs). In this work, the electronic structure and optical properties of fluoranthene, benzo[k]fluoranthene, and their derivatives have been studied using quantum chemical methods. The ground-state structures were optimized using the density functional theory (DFT) methods. The lowest singlet excited state was optimized using time-dependent density functional theory (TD-B3LYP) and configuration interaction singles (CIS) methods. On the basis of ground- and excited-state geometries, the absorption and emission spectra have been calculated using the TD-DFT method with a variety of exchange-correlation functionals. All the calculations were carried out in chloroform medium. The results show that the absorption and emission spectra calculated using the B3LYP functional is in good agreement with the available experimental results. Unlikely, the meta hybrid functionals such as M06HF and M062X underestimate the absorption and emission spectra of all the studied molecules. The calculated absorption and emission wavelength are more or less basis set independent. It has been observed that the substitution of an aromatic ring significantly alters the absorption and emission spectra.  相似文献   

12.
使用密度泛函理论(DFT)B3LYP/6-31G(d)方法优化得到了3(5)-(9-蒽基)吡唑及其衍生物的基态(S0)分子结构, 使用单激发组态相互作用(CIS)/6-31G(d)方法优化得到这些分子的第一单重激发态(S1)的几何结构, 并使用含时密度泛函理论(TD-DFT)B3LYP/6-311++G(d,p)方法计算了它们的吸收和发射光谱. 计算结果表明, 与3(5)-(9-蒽基)吡唑相比, 无论取代基是吸电子基团还是供电子基团, 衍生物的吸收和发射峰均发生红移, 并且当取代基―R=―BH2, ―CCl3, ―CHO, ―NH2时衍生物有较长的吸收波长和发射波长.  相似文献   

13.
The ground and excited state properties of luciferin (LH2) and oxyluciferin (OxyLH2), the bioluminescent chemicals in the firefly, have been characterized using density functional theory (DFT) and time dependent DFT (TDDFT) methods. The effects of solvation on the electronic absorption and emission spectra of luciferin and oxyluciferin were predicted with a self‐consistent isodensity polarized continuum model of the solvent using TDDFT. The S0→S1 vertical excitation energies in the gas phase and in water were obtained. Optimizations of the excited state geometries permitted the first predictions of the fluorescence spectra for these biologically important molecules. Shifts in both of the absorption and emission spectra on proceeding from the gas phase to aqueous solution were also predicted.  相似文献   

14.
用密度泛函理论(DFT)B3LYP方法, 对非金属原子和金属原子分别采用6-311+G(d,p)基组和LANL2DZ基组, 计算并分析了(+)-儿茶素(Cc, C15H14O6)及其与金属形成的配合物分子(M-Cc, M=Ca, Zn, Cd, Cu, Al, Cr)的几何构型、红外光谱和反应活性的异同. 计算结果表明, M-Cc的分子结构、红外光谱与反应活性均不同于其前体Cc. 形成金属配合物后, 取代基团及结构的改变使得红外光谱有所差异. 前线分子轨道及概念DFT指数计算结果显示, 一些M-Cc体系的反应活性要强于Cc单体. 金属离子的不同使得配合物的各指数有所差异. 这些结果将为进一步认识(+)-儿茶素及其相关化合物的结构、红外光谱和反应活性提供有益启示.  相似文献   

15.
The purpose of this work is to provide an in-depth interpretation of the optical and electronic properties of a series of phosphole derivatives, including 2,5-diphenylthiooxophosphole (2a), 2-phenyl-5-biphenylthiooxophosphole (3a), 2-phenyl-5-stilbenylthiooxophosphole (4a), 2,5-dithienylthiooxophosphole (2b), 2-thienyl-5-biphenylthiooxophosphole (3b), 2-thienyl-5-stilbenylthiooxophosphole (4b), and dibenzophosphole 1. These thiooxophospholes show great potential for application in OLEDs as efficient red emitters due to the tuning of the optical and electronic properties by the use of various substituents at the 2,5-positions of the phosphole ring. The geometric and electronic structures of the oligomers in the ground state were investigated using density functional theory (DFT) and the ab initio HF, whereas the lowest singlet excited states were optimized with ab initio CIS. To assign the absorption and emission peaks observed in the experiment, we computed the energies of the lowest singlet excited states with time-dependent DFT (TD-DFT). All DFT calculations were performed using the B3LYP functional and the 6-31G (d) basis set. The results show that the HOMOs, LUMOs, energy gaps, ionization potentials, and electron affinities for the phosphole derivatives are significantly affected by varying the phosphole ring substituents at the 2,5-positions, which favor the hole and electron injection into OLEDs. The absorption and emission spectra exhibit red shifts to some extent [the absorption spectra: 339.63 (1)<358.65 (2a)<373.77 (3a)<443.89 nm (4a) and 403.03 (3b)<449.11 (2b)<460.19 nm (4b); the emission spectra: 418.42 (1)<513.62 (2a)<556.51 (3a)<642.59 nm (4a) and 568.31 (2b)<631.11 (3b)<647.35 nm (4b)] and the Stokes shifts are unexpectedly large ranging from 78 to 228 nm resulting from a more planar conformation of the excited state for the phosphole derivatives.  相似文献   

16.
The FTIR and FT-Raman spectra of 1-bromo 4-fluoronaphthalene have been recorded in the regions 4000-100cm(-1) and 3500-100cm(-1), respectively. The spectra were interpreted with the aid of normal coordinate analysis based on DFT (density functional theory) using standard B3LYP/6-311+G** basis set combination for the most optimized geometry. Normal coordinate calculations performed with the DFT force field and subsequently corrected by a recommended set of scale factors, yielded fairly good agreement between observed and calculated frequencies. On the basis of the comparison between calculated and experimental results, assignments of fundamental modes were examined.  相似文献   

17.
This work deals with the vibrational spectroscopy of succinimide and N-bromosuccinimide. The mid and far FTIR and FT-Raman spectra were measured in the condensed state. The fundamental vibrational frequencies and intensity of vibrational bands were evaluated using density functional theory (DFT) using standard B3LYP/6-31G(*) and B3LYP/6-311+G(**) methods and basis set combinations. The vibrational spectra were interpreted, with the aid of normal coordinate analysis based on a scaled quantum mechanical force field. The infrared and Raman spectra were also predicted from the calculated intensities. Comparison of simulated spectra with the experimental spectra provides important information about the ability of the computational method to describe the vibrational modes. Unambiguous vibrational assignment of all the fundamentals were made using the total energy distribution (TED).  相似文献   

18.
宁攀  赵建想 《化学研究》2013,(5):493-500
应用密度泛函理论,在B3LYP/6-31G(d)和CAM-B3LYP/6-31G(d)水平上优化了α-联噻吩体系H(C4H2S)n H(n=213)的基态几何构型;与此同时,利用TD-B3LYP方法计算了H(C4H2S)n H的吸收光谱,得到了其垂直激发能和体系大小n的解析表达式;并采用TD-CAM-B3LYP方法研究了其发射光谱.研究表明,H(C4H2S)n H的基态结构呈现三种构型:螺旋上升型、环型和稍有弯曲的带状结构;其中前两种构型是顺式结构,最后一种构型是反式结构;环型结构具有C2对称性,其他两种结构具有C1对称性.此外,其吸收光谱和发射光谱计算值与实验值吻合.  相似文献   

19.
采用密度泛函(DFT)和含时-密度泛函(TD-DFT)方法研究二苯胺基团对一类Pt(Ⅱ)配合物(M1~M3)光学性质的调控。通过与实验合成的分子对比,揭示苯胺基团取代位置和数量对电子结构和光学性质的调控规律。引入苯胺基团可有效地增大金属和配体的π共轭性。逐渐增多苯胺基团导致M3分子可以有效地增大吸收光谱的强度和金属到配体的电荷转移(MLCT)占比有利于金属对光的吸收和自旋轨道耦合。M1~M3的发射峰在602~630 nm,发射光谱归属为3MLCT和配体之间的电荷转移(3LLCT)。通过对非辐射跃迁过程,即T1(3MLCT)→TS→金属中心三重态3MC(d-d)的研究,发现当二苯胺取代基团引入位置可以有效地增大分子内空间位阻时,形成S0和T1的系间交叉MECP能量变得更高,从而抑制了非辐射的概率,有利于发光性能提高。  相似文献   

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