2-(2-氨基-3-吡啶基)-苯并咪唑的合成、晶体结构和荧光特性研究

在合成2-(2-氨基-3-吡啶基)-苯并咪唑的基础上,利用NMR(1H、13C、COSY、HSQC和HMBC)、MS、IR和UV进行了详细表征;通过X-ray单晶衍射仪测定了该化合物的晶体结构,实验结果表明该晶体属于三方晶系(空间群R3,a=1.833 7(3)nm,b=1.833 7(2)nm,c=1.777 7(4)nm,V=5.176 4(15)nm3,Z=18),很好地支持了波谱表征的结果。同时,结合密度泛函计算,研究了2-(2-氨基-3-吡啶基)-苯并咪唑的荧光光谱。结果表明,化合物的双荧光不是由同一种异构体发射的,而是来源于不同异构体:长波区500~600 nm的荧光由K构型发射,短波区350~450 nm的发射由异构体E1和E2共同产生,理论预测的光谱与实验一致。     

溶剂效应和取代基效应对2-(2-氨基苯基)苯并噻唑光谱性质及激发态分子内质子转移的影响

合成了多种2-(2-氨基苯基)苯并噻唑(APBT)氨基氢原子被供电子及吸电子基团取代的衍生物, 并用紫外光谱﹑荧光光谱等方法和密度泛函理论(DFT)计算研究了溶剂效应和取代基效应对衍生物的光谱性质及激发态分子内质子转移(ESIPT)的影响规律. 结果表明, 相比于非极性溶剂环己烷, 随溶剂极性的增加及APBT-溶剂分子间氢键的形成, APBT的紫外-可见最大吸收峰和荧光最大发射峰均发生了一定程度的红移, 并对APBT的ESIPT产生了影响. 在APBT分子的氨基氮原子上引入不同的吸电子或斥电子取代基, 对氮原子的电荷性质有较大的影响. 在环己烷溶剂中, 甲基取代后的APBT仅有单重荧光发射峰, 体系未发生ESIPT过程; 而COCH₂Cl等吸电子基团能促进APBT的ESIPT, 其荧光发射光谱出现了明显的双重峰, 表明体系发生了激发态分子内质子转移反应. 量子化学的理论计算较好地验证了光谱实验结果.     

两种4-氨基安替比林席夫碱-Pt(Ⅱ)配合物电子光谱性质的理论研究

采用密度泛函理论(DFT),在PBE0/6-31+G(d)-LANL2DZ水平下,对两种含有不同取代基的4-氨基安替比林席夫碱-Pt(Ⅱ)配合物A和B的几何构型、前线分子轨道及其分布特征进行理论计算.在优化构型的基础上,用含时密度泛函理论(TD-DFT)在相同水平下对上述配合物进行电子吸收光谱研究.计算还考虑了二氯甲烷溶剂对电子结构和光谱性质的影响.结果表明,配合物A和B的最强吸收波长分别来自于HOMO→LUMO和HOMO-5→LUMO的跃迁,以上跃迁存在明显的分子内电荷转移的特征.此外,在4-氨基安替比林配体上引入强的给电子基团-N(CH3)2,配合物A的最大吸收波长相对于配合物B发生了红移现象.     

2,6-二(2-羟基苯乙烯基)-4-甲基均三嗪的合成与性质研究

设计合成了以三嗪基团为骨架的化合物2,6-二(2-羟基苯乙烯基)-4-甲基均三嗪(M1),利用核磁共振H谱和C谱对其结构进行了表征;并对目标化合物在甲醇和乙醚中的紫外,荧光光谱进行了研究.利用量子化学密度泛函理论的B3LYP方法,在6-311+G*水平上,对标题化合物分子构型进行了理论计算.通过实验发现随着溶剂极性增加,紫外吸收峰和荧光光谱的发射峰都发生红移,同时得到的计算光谱数值与实验值吻合较好.     

2-氨基苯并噻唑的结构及激发态质子转移动力学

通过傅里叶变换红外光谱（FTIR）、傅里叶变换拉曼（FT-Raman）和488 nm拉曼光谱,结合密度泛函理论（DFT）计算研究了2-氨基苯并噻唑（ABT）在晶态和溶剂中的二聚体结构,并解释了质子性溶剂中ABT二聚体与溶剂分子间的氢键作用.电子光谱实验揭示了ABT二聚体的光物理和光化学反应;紫外吸收和荧光发射光谱结果表明,溶剂、激发波长和pH值对ABT二聚件激发态衰变具有调控作用;含时密度泛函理论（TD-DFT）解释了ABT二聚体双荧光现象,提出了高激发态的质子转移机理.     

7-吡啶吲哚同分异体结构与电子光谱性质的理论研究

运用密度泛函理论对7-吡啶吲哚可能存在的构型进行优化,计算异构体的几何构型、电子结构、前线分子轨道;应用含时密度泛函理论计算了异构体b,c和e的电子光谱性质以及溶剂效应对光谱性质的影响.结果表明,溶剂极性的增加使b的电子光谱蓝移,而c和e的电子光谱红移,且溶剂极性对最大吸收波长影响幅度较小.前线分子轨道分析,表明该类化合物的主要吸收光谱主要对应于分子中的HOMO→LUMO电子跃迁,且为π→π*跃迁.     

5-甲基-3-硝基-4-异噁唑甲酰腙分子光谱的理论计算

采用B3LYP/3-21+G*方法,对5-甲基-3-硝基-4-异噁唑甲酰腙及其取代物的基态结构进行优化,用间略微分重叠(ZINDO)计算其电子吸收光谱(UV-Vis);用CIS/STO-3G方法优化其最低激发单重态的几何结构,用密度泛函理论方法TD-PBEPBE/6-311+G-water计算其发射光谱.同时还探讨了取代基的种类(如—CH3,—C2H5,—NH2等推电子基,—NO2,—Cl,—COOH等吸电子基)、取代基的位置(如邻位取代、间位取代、对位取代)和溶剂等因素对其衍生物电子光谱性质的影响.结果表明:标题物的模拟UV-Vis 3个光谱峰和其荧光发射最大值均与标题物分子的实验值基本符合;改变取代基的种类和位置等均可精细地调控标题物的光谱峰位和强度.     

间位取代卟啉及其锌卟啉的电子吸收光谱

取代的卟啉类衍生物在气敏传感器方面具有广泛的应用前景.本文采用了密度泛函理论(DFT)和含时密度泛函理论(TD-DFT)研究了四种不同取代基的卟啉衍生物(meso位四硝基苯基/四氨基苯基卟啉(NO2PP,NH2PP)及其相应的锌金属卟啉衍生物(NO2ZnPP,NH2ZnPP))的紫外和近紫外光谱特征.利用两种不同的交换相关泛函(广义梯度近似泛函(PBE)和杂化密度泛函(B3LYP))优化了上述四种物质的结构,并应用TD-DFT计算了相应的电子激发能量和振动强度.结果表明,取代卟啉的吸收光谱与大量的电子跃迁有关;与B3LYP泛函预测的光谱相比,PBE泛函所得B带以及Q带的波长位置与实验值更为接近.另外,计算所得硝基取代基卟啉的B带相对于氨基取代基卟啉的B带发生了红移,这与实验现象也保持一致.由于卟啉衍生物的三重激发态在电子转移中有很重要的应用,因此在PBE/6-31G(d)水平上计算了四种物质的最低三重激发态能量,分别为1.426、1.469、1.608和1.581eV.     

2-(2-羟基-5-氨苯基)苯并咪唑与氨基卟啉能量转移的研究

采用紫外光谱法和荧光光谱法研究了二氯甲烷溶液中2-(2-羟基-5-氨基苯基)苯并咪唑(NH_2-HBI)和5-(4-氨基)苯基-10,15,20-三苯基卟啉(NH_2-TPP)两分子之间的能量转移作用,测定了NH_2-HBI与NH_2-TPP作用的结合比及能量转移参数.结果表明,在光的激发作用下,形成了以NH_2-HBI为能量供体、NH_2-TPP为能量受体的荧光共振能量转移(FRET)体系,同时发生了NH_2-HBI激发态分子内质子转移(ESIPT)与FRET的耦合作用, NH_2-HBI分子的醇式构型与酮式构型的荧光都被部分的猝灭,而NH_2-TPP的荧光却明显的增强.两分子形成了1∶1的供体-受体作用分子对,体系的FRET能量转移效率(E_(FRET))为0.114,临界能量转移距离(R_0)为2.293nm,供-受体之间的距离(r)为3.227 nm.     

6-甲基-4-羟基嘧啶单体及二聚体激发态质子转移异构化反应及光谱的理论研究

采用ab initio HF理论的组态相关CIS方法和连续溶剂模型PCM, 分别在6-311+G*和6-31G水平上研究了6-甲基-4-羟基嘧啶单体及二聚体激发态质子转移的异构化反应; 对其反应势能面的研究发现, 单体基态和激发态的异构化反应一起可以形成四能级的分子电子体系, 而二聚体的却不能, 由此解释了单体和二聚体的紫外吸收光谱和荧光发射光谱均对应于酮式构型的原因. 利用混合含时密度泛函TD/MPW1PW91理论方法在溶剂存在下计算了标题物质的紫外吸收光谱和荧光发射光谱.     

The calculation of ground and excited state molecular polarizabilities: A simple perturbation treatment

Second order perturbation theory has been coupled with the CNDO/S CI method of Del Bene and Jaffé to calculate the ground and excited state polarizabilities of various molecules. It is found that this treatment produces reasonably good polarizabilities with great computational ease.     

Is the ˜c state of CH2 linear or bent?

The ˜c state of CH₂ is found to be bent at the highest levels of theory used in this work, but the energy difference between the linear and bent geometries is only about 10 cm⁻¹. Improving the basis set or correlation treatment favors the linear geometry over the bent, thus it is impossible to definitively determine if the ˜c state has a barrier in its bending potential. If there is a barrier, it is clear that it will be so small that the ˜c state will be quasilinear. Received: 3 September 1996 / Accepted: 23 September 1996     

Enhancement of luminescence properties in Er3+ doped TeO2-Na2O-PbX (X=O and F) ternary glasses

An enhancement of luminescence properties in Er3+ doped ternary glasses is observed on the addition of PbO/PbF2. The infrared to visible upconversion emission bands are observed at 410, 525, 550 and 658 nm, due to the 2H9/2-->4I15/2, 2H11/2-->4I15/2, 4S3/2-->4I15/2, 4F9/2-->4I15/2 transitions respectively, on excitation with 797 nm laser line. A detailed study reveals that the 2H9/2-->4I15/2 transition arises due to three step upconversion process while other transitions arise due to two step absorption. On excitation with 532 nm radiation, ultraviolet and violet upconversion bands centered at 380, 404, 410 and 475 nm wavelengths are observed along with one photon luminescence bands at 525, 550, 658 and 843 nm wavelengths. These bands are found due to the 4G11/2-->4I15/2, 2P3/2-->4I13/2, 2H9/2-->4I15/2, 2P3/2-->4I11/2, 2H11/2-->4I15/2, 4S3/2-->4I15/2, 4F9/2-->4I15/2 and 4S3/2-->4I13/2 transitions, respectively. Though incorporation of PbO and PbF2 both enhances fluorescence intensities however, PbF2 content has an important influence on upconversion luminescence emission. The incorporation of PbF2 enhances the red emission (658 nm) intensity by 1.5 times and the violet emission (410 nm) intensity by 2.0 times. A concentration dependence study of fluorescence reveals the rapid increase in the red (4F9/2-->4I15/2) emission intensity relative to the green (4S3/2-->4I15/2) emission with increase in the Er3+ ion concentration. This behaviour has been explained in terms of an energy transfer by relaxation between excited ions.     

时间域方法分析镍卟啉的共振拉曼强度与S2激发态结构

研究了入射光波长与S0→S2跃迁共振的情形下,卟啉镍配合物（NiP）的振动拉曼光谱。用时间域方法计算了NiP的共振拉曼强度和吸收光谱。结果表明,相对于基态,S2态NiP的分子构型沿着ν8和ν2简正坐标有较大的位移。这些简正坐标主要涉及卟啉环的CαCm键和CβCβ键伸缩运动,以及CαCmCα变角运动。与基态相比, S2态的CβCβ、 CαCm和CαN键分别增大0.27、 0.14、 0.07 pm,而CαCβ键则减小0.20 pm,与前人的赝势分子轨道计算（SPMO）结果相近。还从RR强度角度讨论了S2态的Jahn-Teller畸变。     

从Hückel分子轨道理论导出激发态周环反应的奇偶定则

本文从Huckel分子轨道理论,导出激发态周环反应的奇偶定则。在推导中Huckel久期行列式的非零元均视为反应坐标的函数,对其数值不作特殊假定。本文的推导也有助于对周环反应的Mobius-Huckel结构理论获得进一步的了解。     

Excited state properties of neutral, anionic and cationic 1,1-disubstituted 2,3,4,5-tetraphenylsiloles: A quantum chemical characterization

Structure, electronic states, photoluminescence, and carries transport properties of 1,1-disubstituted 2,3,4,5-tetraphenylsiloles for light-emitting diodes were investigated experimentally [G. Yu, et al, J. Am. Chem. Soc. 2005, 127, 6335], and the excellent electroluminescent (EL) properties of them have been found. In this paper, excited state properties of neutral, anionic and cationic 1,1-disubstituted 2,3,4,5-tetraphenylsiloles are studied with quantum chemistry method as well as the 3D real space analysis methods. The transition densities of neutral, anionic and cationic 1,1-disubstituted 2,3,4,5-tetraphenylsiloles show that the orientations and strengths of dipole moments the neutral, anionic and cationic ones are significantly different, where the neutral 1,1-disubstituted 2,3,4,5-tetraphenylsiloles show the Frenkel character; while the anionic and cationic 1,1-disubstituted 2,3,4,5-tetraphenylsiloles show the plasmon character. The charge difference densities of neutral, anionic and cationic 1,1-disubstituted 2,3,4,5-tetraphenylsiloles reveal the important diversity of the orientations and the results of intramolecular charge transfer (ICT). The theoretical results also reveal the contribution of the substituents at the 1,1-position to the neutral and charged excited state properties of 2,3,4,5-tetraphenylsiloles. The calculated results are consistent with the experimental results, and further provide the insight of understanding to the excited state properties of neutral, anionic and cationic 1,1-disubstituted 2,3,4,5-tetraphenylsiloles.     

Theoretical studies on structures and spectroscopic properties of bis-cyclometalated iridium complexes [Ir(ppy)2X2]

The electronic structures and spectroscopic properties of a series of mixed bis-cyclometalated iridium(III) complexes [Ir(ppy)₂X₂]⁻ (X = CN, 1; X = NCS, 2; X = NCO, 3; ppy = 2-phenylpyridl) were investigated at the B3LYP/LANL2DZ and CIS/LANL2DZ levels. The calculated geometry parameters in the ground state are well consistent with the corresponding experimental values. The HOMO of 1 is dominantly localized on Ir atom and ppy ligand, but the HOMO of 2 and 3 have significant X ligand composition. Under the TD-DFT level with PCM model, the absorption and phosphorescence in CH₂Cl₂ media were calculated based on the optimized geometries in the ground and excited states, respectively. The lowest-lying absorption of 1 at 403 nm is attributed to {[d_x²-y²(Ir)+d_xy(Ir)+π(ppy)]→[π^∗(ppy)]} transition with metal-to-ligand and intraligand charge transfer (MLCT/ILCT) transition characters, whereas those of 2 (449 nm) and 3 (475 nm) are related to {[d_x²-y²(Ir)+d_xy(Ir)+π(ppy)+π(NCS/NCO)]→[π^∗(ppy)]} transition with MLCT/ILCT and ligand-to-ligand charge transfer (LLCT) transition characters. The phosphorescence of 1 at 466 nm can be described as originating from ³{[d_x²-y²(Ir)+d_xy(Ir)+π(ppy)][π^∗(ppy)]} excited state, while those of 2 (487 nm) and 3 (516 nm) originate from ³{[d_x²-y²(Ir)+d_xy(Ir)+π(ppy)+π(NCS/NCO)][π^∗(ppy)]} excited states. The calculated results showed that the transition character of the absorption and emission can be changed by adjusting the π electron-accepting abilities of the X ligands and the phosphorescent color can be tuned by altering the X ligands.     

Si2分子基态和低激发态的电子结构

本文用abinitioSOCI／MCSCF／／HF／DH＋d方法计算得到了Si2分子的基态和八个激发态的平衡几何构型、总能量、谐振动频率、零点能以及各个态的势能曲线．讨论了各态键长随电子组态的变化关系，指出了成健轨道中。电子数的增加，是引起键长及谐振动频率变化的重要因素·其中3Πg，5∑；3△u，3∑，未见有关文献报导由于硅藻合物的重要应用价值，人们已对其进行了一些实验和理论研究h，’」．以前的研究主要是讨论其成键性质．由于St。分子结构的特殊性，要想全面了解其成键性质，不仅要研究其基态的电子结构，而且还要研究其激发态的电…     

Theoretical studies upon the electronic structures and spectroscopic properties for a series of luminescent terpyridyl platinum(II) phenylacetylide complexes

A comprehensive calculations were carried out to get a deep insight into the ground- and excited-state electronic structures and the spectroscopic properties for a series of [Pt(4-X–trpy)CCC₆H₄R]⁺ complexes (trpy = 2,2′,6′,2″-terpyridine; X = H, R = NO₂ (1), Cl (2), C₆H₅ (3) and CH₃ (4); R = Cl, X = CH₃ (5) and C₆H₅ (6)). MP2 (second-order Møller–Plesset perturbation) and CIS (single-excitation configuration interaction) methods were employed to optimize the structures of 1–6 in the ground and excited states, respectively. The investigation showed that substituted phenylacetylide and trpy ligands only give rise to a small variation in geometrical structures but lead to a sizable difference in the electronic structures for 1–6 in the ground and excited states. The introduction of electron-rich groups into the phenylacetylide and/or terpyridyl ligands produces two different low-lying absorptions for 1 and 2–6, i.e., Pt(5d) → π^*(trpy) metal-to-ligand charge transfer (MLCT) mixed with π → π^*(CCPh) intraligand charge transfer (ILCT) for 1 and Pt(5d)/π(CCPh) → π^*(trpy) charge transfer (MLCT and LLCT) for 2–6. Remarkable electronic resonance on the whole Pt–CCPh–NO₂ moiety for 1 may be responsible for the difference. Solvatochromism calculation revealed that only LLCT/MLCT transitions showed the solvent dependence, consistent with the experimental observations.     

Regiospecific photoisomerization of fluorinated (E,E)-1,4-diphenyl-1,3-butadienes

Photoisomerization of five fluorinated E,E-1-(R-phenyl)-4-phenyl-1,3-butadienes in solution (R = 1: p-monofluoro, 2: m,m′-difluoro, 3: m,m′,p-trifluoro, 4: o,o′,m,m′-tetrafluoro, 5: o,o′,m,m′,p-pentafluoro) was investigated via direct irradiation. Our results indicated that cis-trans photoisomerization of the fluorinated 1,4-diphenyl-1,3-butadienes in the excited singlet state took place exclusively at the CC bonds closer to the fluorine substituents.