3,9-咔唑聚合物基态和激发态性质的理论研究

用密度泛函B3LYP方法对3,9-咔唑低聚物[(3,9-carbazole)n(n=1,2,3,4,6,8)]体系进行了全优化, 计算得到电离能、电子亲合势、空穴抽取能及电子抽取能等相关能量, 用ZINDO和TD-DFT方法计算得到吸收光谱; 分析了各种能量的变化及光谱规律. 用外推法由低聚物分子的各种性质与聚合度n相联系得到高聚物的性质, 将所得结果与2,7-咔唑(2,7-carbazole)及类似聚合物进行了比较分析. 结果表明, 3,9位聚合的咔唑整体共轭程度降低, 光谱蓝移, 其IP值和聚芴相近, 可以作为空穴接受材料应用于多层电子荧光器件的空穴传输层. 用CIS方法进行优化得到部分分子的S1激发态结构, 用ZINDO和TD-DFT方法得到对应的发射光谱.     

3-(3’-吡啶基)-6-芳基-1,2,4-三唑并[3,4-b]-1,3,4-噻二唑衍生物基态和激发态性质

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.     

3-(3′-吡啶基)-6-芳基-1，2，4-三唑并[3，4-b]-1，3，4-噻二唑衍生物基态和激发态性质

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.     

六硝基六氮杂异伍兹烷结构和性质的理论研究

用abinitio和DFT方法,分别在HF/6-31G^*和B3LYP/6-31G^*水平下全优化计算了高能量密度材料六硝基六氮杂异伍兹烷(HNIW)的α(γ),β和ε型构象的分子几何构型、电子结构、IR谱和298～1000K温度下的热力学性质,细致分析比较了两种方法和相关的实验结果。理论计算几何参数与实验值相一致。分子中N—N键较长,N—N键Mulliken集居数较小,预示该键为热解和起爆的引发键。所得的IR谱形符合实验、指纹区频率与实验的平均绝对差值小于45cm^-1。由前线MO能级及其差值预示的热力学稳定性次序[ε＞α(γ)＞β]与实验排序相吻合。     

氮杂联苯乙烯系列衍生物的二阶非线性光学性质的理论研究

新型高非线性光学活性生色团分子的设计与探索已成为近来工作的焦点 [1] .化学家们 [2～ 9]研究了大量具有π电子结构和有分子内电子转移的有机化合物如推拉苯乙烯、 Schiff碱、偶氮苯、取代吡啶、噻吩乙烯等体系的二阶非线性光学特性 ,发现这些推拉共轭体系的共轭链长增加均导致二阶非线性极化率 β增大 ,紫外光谱红移 ,透明性降低 .本文研究推拉氮杂苯乙烯及二苯乙烯系列衍生物的二阶非线性光学性质 .结果表明 ,对于苯乙烯和二苯乙烯衍生物 ,引入嘧啶环既提高了二阶非线性光学系数 ,又不影响材料的透明性 ,是很有前途的二阶非线性光学候…     

三氮杂苯-水氢键复合物的结构与性质

使用密度泛函理论B3LYP方法对三氮杂苯-水氢键复合物的基态结构与相互作用进行理论研究. 结果表明1,2,3-三氮杂苯-水, 1,2,4-三氮杂苯-水和1,3,5-三氮杂苯-水复合物基态分别具有Cs, Cs和C₁对称性和强的氢键相互作用, 经基组重叠误差和零点振动能校正后的相互作用能分别为–17.83, –17.38和–13.55 kJ/mol. 三氮杂苯-水复合物中, N∙∙∙H—O氢键的形成使水的H—O对称伸缩振动频率明显红移. 同时使用含时密度泛函理论研究了三氮杂苯单体及其与水形成的氢键复合物的第一¹(n, π^*)激发态的垂直激发能.     

深度脱硫噻吩衍生物的电子和空间性质理论研究

我们采用从头计算的密度泛函理论方法在B3LYP水平上,其中H原子采用3-21G基组,C原子采用6-31G(d)基组,S原子采用6-31G (d)基组对2-甲基噻吩,苯并噻吩,2-甲基苯并噻吩,二苯并噻吩,4-甲基-二苯并噻吩,4,6-二甲基二苯并噻吩等噻吩衍生物进行了几何优化．研究结果表明电子性质可影响噻吩衍生物的加氢脱硫活性,但空间因素对噻吩衍生物的加氢脱硫活性影响很大,从而证实了提高噻吩衍生物加氢脱硫活性方案的可行性．     

二氮杂苯－水氢键复合物结构性质的理论研究

使用密度泛函理论B3LYP方法和从头算MP2方法优化二氮杂苯－水复合物的基态氢键结构和相互作用能的计算。结果表明,邻二氮杂苯－水,间二氮杂苯－水,对二氮杂苯－水复合物具有强的N∙∙∙H─O氢键相互作用,经基组重叠误差和零点能校正后的氢键相互作用能分别为-20.99, -16.73 和-15.31 kJ/mol,氢键的形成使水的H─O对称伸缩振动频率明显红移（减小）。自然键轨道NBO分析显示,氢键的形成,分子间电荷转移分别为0.0316 e,0.0255 e 和0.0265 e。另外,使用含时密度泛函理论TD-DFT (TD-B3LYP)方法计算了二氮杂苯单体与氢键复合物的第一单重态(n, p^*)激发态的垂直激发能。     

六硝基芪衍生物的红外光谱和热力学性质的理论研究

用量子化学密度泛函理论方法,在B3LYP/6-31G*水平下,对六硝基芪衍生物进行了几何构型全优化和电子结构计算。通过振动分析,求得它们的红外光谱并作归属。将理论计算IR谱与已知实验结果进行比较,表明本文所提供的计算结果是可靠的。对谐振频率以0.96进行标度后基于统计热力学原理求得它们的热力学性质,探讨了热力学性质随硝基数、氨基数、羟基数和温度变化的规律,发现有很好的线性关系,体现了很好的基团加和性。     

1,2,3-三氮杂苯-水簇复合物氢键结构与性质的理论研究

在B3LYP/6-31 G**水平上对1,2,3-三氮杂苯和水形成1∶1,1∶2和1∶3复合物的基态氢键结构进行几何优化和性质计算,结果表明复合物之间存在较强的氢键作用。氢键的形成使水分子中H-O键振动频率减小(红移)。NBO分析表明,最稳定的1∶1,1∶2和1∶3复合物发生分子间电荷转移总量分别为0.0222e,0.0261e和0.0273e。     

High level of ab initio and density functional theory computational study of structural and energetic properties of tetrafluorhydrazine rotamers

The HF, MP2, MP3, MP4, and QCISD ab initio methods were compared with local, hybrid, and gradient-corrected density functional theory (DFT) methods for computing structures and energies of N2F4 rotamers. In all DFT calculations 6-311 + G(2d) basis set was used. The generated structures energies of trans- and gauche-N₂F₄ rotamers, and their dissociation energies to nitrogen difluoride were compared with experimental data. Suitable hybrid and gradient-corrected DFT methods for determining structures and energies for these and similar molecular systems were discussed.     

Ab initio and density functional theory calculations of molecular structure and vibrational spectrum of ethyl azidoacetate

Here we report ab initio and density functional results for molecular properties of ethyl azidoacetate (N₃CH₂COOC₂H₅) and for the corresponding singly ionized structure (N₃CH₂COOC₂H₅⁺). Ab initio ionization energies based on Koopmans’ theorem are in excellent agreement with the experimental data from ultraviolet photoelectron spectroscopy. DFT adiabatic energy differences between neutral and ionized structures are very sensitive to electronic correlation effects and are not in very good agreement with experiment. The results for the structure and vibrational frequencies are compared with the experimental data of related molecular structures.     

密度泛函理论和从头算方法对四唑负离子的比较研究

运用多种密度泛函理论(DFT)方法和从头算(abinitio)方法研究了四唑负离子的分子几何、电子结构、红外光谱和热力学性质.结果表明,B3LYP-DFT法与MP2-abinitio法计算结果较吻合,故可用于对四唑衍生物及其配合物的系统研究.     

Thermochemistry of the higher chlorine oxides ClOx (x=3, 4) and Cl2Ox (x=3–7)†

Heats of formation for ClO₃, ClO₄, Cl₂O₃, Cl₂O₄, Cl₂O₅, Cl₂O₆ and Cl₂O₇ molecules are determined at the B3LYP, B3PW91, mPW1PW91 and B1LYP levels of the density functional theory employing a series of extended basis sets, and using Gaussian-3 model chemistries. Modified Gaussian-3 calculations, which employ accurate B3LYP/6-311+G(3d2f) molecular geometries and vibrational frequencies, were also performed. Heats of formation were calculated from both total atomization energies and isodesmic reaction schemes. The latter method in conjunction with Gaussian-3 models leads to the most reliable results. The best values at 298 K for ClO₃, ClO₄, Cl₂O₃ and Cl₂O₄ as derived from an average of G3//B3LYP and G3//B3LYP/6-311+G(3d2f) calculations are 43.1, 54.8, 31.7 and 37.4 kcal mol⁻¹. From calculations carried out at the G3(MP2)//B3LYP and G3(MP2)//B3LYP/6-311+G(3d2f) levels, heats of formation for Cl₂O₅, Cl₂O₆ and Cl₂O₇ are predicted to be 53.2, 52.2 and 61.5 kcal mol⁻¹. All best values are reproduced within 1 kcal mol⁻¹ by using mPW1PW91/6-311+G(3d2f) isodesmic energies. Enthalpy changes for relevant Cl–O bond fission reactions are reported. Comparisons with previous thermodynamics data are made.     

Elucidating ultrafast nonradiative decay of photoexcited uracil in aqueous solution by ab initio molecular dynamics

Nonradiative decay of the photoexcited RNA base uracil has been studied in fully explicit aqueous solution using nonadiabatic ab initio molecular dynamics. Detailed comparison of the time-dependent nonadiabatic transition probability with specific molecular vibrational motions provides insight into the mechanism of the ultrafast internal conversion. From a monoexponential fit to the excited state ensemble population, the lifetime of the first electronically excited ππ^* singlet state has been determined to be 359 fs. Additional, reference, nonadiabatic simulations have been carried out in the gas phase, pinpointing the effects of the solvent on the photophysics of uracil. The gas phase excited state lifetime is calculated to be 608 fs, somewhat longer than in solution. In terms of excitation energies and geometrical parameters, the differences between gas phase and aqueous solution are found to be generally small. A notable exception is the excited state out-of-plane torsional motion about the CC double bond, which appears severely damped by the solvent. Moreover, hydrogen bond interactions between the uracil oxygens and the solvent hydrogens are seen to enhance internal conversion.     

杂硼原子簇XB6+ (X=C,Si, Ge,Sn, Pb)的稳定性和芳香性

利用从头算MP2方法和密度泛函理论B3LYP和B3PW91方法, 研究了杂硼原子簇XB₆⁺ (X=C, Si, Ge, Sn, Pb)的结构、稳定性及化学键合情况. 对C, Si, Ge, B使用6-311+G(d)基组, 对Sn和Pb使用LANL2DZ赝势基组. 研究结果表明, 具有C_s对称性的假平面XB₆⁺ (X=C, Si, Ge, Sn, Pb)结构是势能面上的全域极小点, 其稳定性要高于C_6v对称性的锥形结构和C₂对称性的假锥形结构. 在B3LYP水平上, 对这些异构体的势能面的极小点进行了自然键轨道(NBO)的分析; 对最稳定构型的最高占据分子轨道(HOMO)和最低空轨道(LUMO)能级差、分子轨道(MO)和核独立化学位移(NICS)进行了计算和讨论. 分析了杂原子和硼原子间、相邻硼原子间的键合情况, 讨论了最稳定构型的芳香性质.     

Frist-principles Band Structures Calculation of Tin-phthalocyanine

We adopt the density function theory with generalized approximation by the Beeke exchange plus Lee-Yang-Parr correlation functional to calculate the electronic first-principles band structure of tin-phthalocyanine （SnPc）. The intermolecular interaction related to transport behavior was analyzed from the F-point wave function as well as from the bandwidths and band gaps. From the calculated bandwidths of the frontier bands as well as the effective masses of the electron and hole, it can be concluded that the mobility of the electron is about two times larger than that of the hole. Furthermore, when several bands near the Fermi surface are taken into account, we find that the interband gaps within the unoccupied bands are generally smaller than those of the occupied bands, indicating that the electron can hop from one band to another which is much easier than the hole. This may happen through electron-phonon coupling for instance, thus effectively yielding an even larger mobility for the electron than for the hole. These facts indicate that in SnPc the electrons are the dominant carriers in transport, in contrast to most organic materials.