2-甲基噻吩光异构化成3-甲基噻吩的理论研究

用CASSCF方法以6-31G基组研究了2-甲基噻吩光异构化为3-甲基噻吩的光化学反应和基态(S₀)及三重激发态(T₁)的相关势能面.反应主要发生在三重态(T₁)上,其间经历了两个双自由基,1个三元环中间体及4个过渡态.沿着反应路径找到了2个T₁/S₀势能面交叉点,其结构都类似于双自由基.在第二个T₁/S₀势能面交叉点附近由T₁向S₀的系间窜越(ISC)最为有利.     

多共振热激活延迟荧光过程的理论研究

本工作借助第一性原理和动力学演化,系统地研究了四个叔丁基-咔唑及吩噻嗪取代的硼-氮化合物(BCz-BN、2PTZ-BN、Cz-PTZ-BN和2Cz-PTZ-BN)的多共振热激活延迟荧光的高效发光机制.结果表明上述分子T₁与T₂间的内转换速率远大于其它辐射与非辐射速率,同时T₂到S₁的反向系间窜越速率也高于T₁到S₁的反向系间窜越速率,因此其多共振热激活延迟荧光过程应遵循T₁→T₂→S₁→S₀的路径.进一步动力学演化表明,T₁与T₂之间的内转换主要发生在演化初期,随着时间的推移,能量逐渐由T₂向S₁转移,并最终在S₁完成荧光发射.上述研究揭示了多共振延迟荧光的微观本质,为未来设计及合成新的多共振热激活延迟荧光分子提供了理论依据.     

硫代樟脑光化学反应的理论研究

运用量子化学方法优化了硫代樟脑的最低5个电子态(S₀, T₁, S₁, T₂和S₂)的结构, 并计算了它们的相对能量. 计算结果表明: S₁, T₁和T₂态的能量非常接近, 而S₂的能量远远高于T₂态, 这与之前对几种小的硫代羰基化合物的研究结论一致. 确定了硫代樟脑分子在T₁态发生β-插入反应和类Norrish II型反应的机理, 计算的势垒相对于S₀的振动零点分别为314.1和332.6 kJ/mol. 在400 nm波长的光的照射下, 分子被激发到S₁态, 此时分子没有足够的能量发生反应, 只能通过内转换回到基态. 当激发光波长在254 nm时, 硫代樟脑分子被激发到S₂态, 这时候体系有了足够的内部能量使反应发生. 实验上已经观察到此激发光波长下, 气态硫代樟脑可以发生β-插入反应和类Norrish II型反应.     

(Ag,Au)/MoS2的电解水性能及等离激元光热作用

MoS₂是电解水体系的一种备受关注的非贵金属析氢催化剂,优化其活性位点是提高其活性的研究重点.采用水热法在三维导电碳布(CC)上合成了二维片状Mo S₂,将反应温度从200℃调至180℃可保留具有更多活性位点的1T相,相应的Mo S₂(180)/CC电极表现出相对更低的析氢过电位.利用电化学方法在Mo S₂(180)/CC上分别沉积Ag和Au纳米粒子,得到Ag/Mo S₂(180)/CC和Au/Mo S₂(180)/CC电极.扫描电子显微镜(SEM)、X射线衍射(XRD)、X射线光电子能谱(XPS)表征结果以及无光照、光照和加热条件下电化学极化曲线、电化学阻抗谱(EIS)和Tafel斜率的测试结果表明,20 nm Ag和30 nm Au的负载及光照条件均可降低析氢过电位和增加电流密度,而体系温升的作用与金属的种类有关.利用COMSOL Multiphysics软件构建Mo S₂,Ag/Mo S₂和Au/Mo S<...     

双核钼(Ⅴ)二乙基二硫代氨基甲酸络合物的歧化离解平衡及其离解常数

由于发生歧化离解,Mo₂O₃(S₂CNEt₂)₄的溶液不遵守Beer定律,我们测定了有关溶液的光吸收性质以及Mo₂O₃(S₂CNEt₂)₄的歧化离解常数,于15℃时数值为2.2×10^-4。     

理论研究二米基硼B(Mes)2位置异构对Ir(III)配合物Ir(ppy)2(acac)的光物理性质的影响

采用DFT/TDDFT方法研究了二米基硼B（Mes）₂基团修饰的一类Ir（ppy）₂（acac）配合物1～3的光物理性质. 计算了电子结构,吸收和发射光谱以及自旋轨道耦合矩阵< T₁^α|H_SOC|S_n >和辐射跃迁速率（k_r）,探讨了取代基位置不同对磷光辐射和非辐射跃迁性质的影响. 研究结果表明：向ppy配体的吡啶环引入B（Mes）₂基团,能够加强金属铱（Ir）与配体乙酰丙酮（acac）的相互作用,减小单-三重态能级差ΔE（S₁-T₁）,提高系间窜跃速率和磷光辐射跃迁速率. 向ppy配体的苯环引入B（Mes）₂基团则增大了S₀与T₁的结构变形和自旋轨道耦合矩阵< S₀|H_SOC|T₁ >,使非辐射跃迁速率增加. B（Mes）₂基团位置异构,导致金属d轨道分裂方式不同,其在三个方向的自旋轨道耦合作用不同,辐射跃迁和非辐射跃迁都随之改变. 从理论上解释了通过对ppy配体的吡啶环修饰可获得高磷光量子产率的原因.     

光合释氧机理的ABEEM/MM/MD和BS-DFT理论研究

建立了S₂态光合释氧络合物（OEC）的原子-键电负性均衡模型（ABEEMσπ）的电荷参数,并使用ABEEM/MM/MD可极化力场的分子动力学模拟和对称性破损的DFT研究了光合作用制造氧气的微观机制.HF/STO-3G（采用此基组的原因请见引用文献）水平下的电荷拟合结果证明了ABEEMσπ模型计算电荷分布的合理性和高效性.MD模拟显示,S₂态Mn₄CaO₅的双向异构化过程伴随Ca上的水分子W3转移至Mn1（III）/Mn4（III）,它很可能作为底物水之一,与O5在S₄态结合产生O₂.基于此,考察了全自旋态下两种异构体形式中O－O键形成的自由基耦合机理.BS-DFT计算结果表明,开立方结构的释氧活性大大优于闭立方结构,金属锰和氧自由基的自旋耦合方式也是反应性的决定性因素,同时,OEC的结构灵活性对于S态循环和光合水分解至关重要.     

发展尿素与丙氨酸二肽相互作用的ABEEM/MM可极化力场

基于ABEEM/MM浮动电荷模型，尝试建立了一个新的可合理描述尿素-丙氨酸二肽-水分子之间相互作用的可极化力场.采用量子力学(QM)ωB97X-D/6-311++G(3df, 2p)//MP2/aug-cc-pVTZ方法对(Urea)(Ala)₂的结构、电荷分布及结合能进行计算，以及HF/STO-3G方法计算电荷分布.构建尿素-丙氨酸二肽-水体系的ABEEM/MM势能函数，基于QM计算结果，优选确定相关参数.结果表明，与QM相比，ABEEM/MM获得的(Urea)(Ala)₂的键长、键角、二面角和结合能的AAD(平均绝对偏差),RMSD(均方根偏差)和RRMSD(相对均方根偏差)分别为0.000 8 nm, 0.001 4 nm, 1.2%;1.36°,1.72°,1.5%;4.10°,5.56°,5.0%;6.07 kJ·mol^-1,6.82 kJ·mol^-1和10.2%,电荷分布的线性相关系数为0.988.将上述势能函数应用于(Ala)₂(Urea)₂...     

氮杂环配体对卤化亚铜配合物发光机制影响的理论研究

为深入探讨卤化亚铜配合物的发光机制，运用密度泛函理论和含时密度泛函理论的计算方法研究了三个结构相似的溴化亚铜配合物(CuBr-py、CuBr-iq、CuBr-nap)。研究结果表明，CuBr-py和CuBr-nap,电子和空穴重叠程度小，导致其ΔE_ST较小；S₁与T₁间的重组能较小，使其可快速地完成反系间窜越过程，实现热活化延迟荧光(TADF)。此外，与CuBr-nap相比，CuBr-py自旋轨道耦合作用强，其磷光速率也较大，因此其具有TADF和磷光双通道发光特性。而CuBr-iq中喹啉环的存在增大了电子和空穴的重叠程度，ΔE_ST增大；同时S₁与T₁间的重组能较大，T₁无法顺利通过RISC过程回到S₁,导致其最终呈现出磷光特性。这些理论计算结果与实验现象一致，且揭示了N杂环配体结构对于卤化亚铜配合物发光机制的影响规律，为设计和合成稳定高效的发光材料提供了有价值的理论指导。     

原子簇化合物[Et4N]2[Mo2O2S2(S2)(S4)]的合成和结构

目前,Mo-S化合物的化学,特别是以多硫基为配体的铟硫化合物的化学是一个活跃的研究领域。这里我们报道含S₂^2-、S₄^2-两种多硫基的二核钼原子簇化合物〔Et₄N〕₂〔Mo₂O₂(S₂)(S₄)(u₃-S)₂]的合成和单晶结构。     

Simulated T ← S spectra of benzaldehydes as a function of the energy gap between the ππ and nπ levels

The T_1,2 ← S₀ spectra of benzaldehydes have been studied as a function of the energy separation between the vibrationless levels. It is shown that the spectra are very complicated in the region of ΔE[T₂⁰(nπ^*)-T₁⁰(ππ^*)] = 250–400 cm⁻¹, reflecting effective vibronic interferences between T₂⁰(0-0) and each of the ν₃₆-ν₃₃ out-of-plane vibrational levels of T₁⁰(ππ^*). The simulated spectra correspond to the observed spectra. In the case of T₁⁰ = ³nπ^* and T₂⁰ = ³ππ^* the spectral change is not so drastic as in the reverse case loc. cit. because the optical intensity generally concentrates in the longest wavelength band, i.e., the origin band of the T₁(nπ^*) ← S₀ transition. The simulation spectra are useful for interpretation of the absorption spectra in similar electronic structure systems of substituted benzaldehydes.     

S2 → S0 fluorescence in an aromatic thioketone, xanthione

In addition to the red phosphorescence (T₁(³ A₂n, π^*) → S₀) xanthione exhibits in solution an emission with a maximum at ≈ 23 000 cm⁻¹ and φ_f(298°) = 5 × 10⁻³. It is shown that this emission is fluorescence from the second excited singlet state (S₂ (¹A₁ π, π^*) → S₀).     

Spectroscopic study of harmane in micelles at 77 K using fluorescent probes

Steady-state and time-resolved emission for spectroscopic techniques at 77 K, and molecular orbital calculations using PM3-MOPAC/93 and HAM/3-CI have been used to study the two forms of harmane, the neutral (HN) and the monoprotonated (HH), in different environments. In hydrophobic media, for (HN), four species were determined and in hydrophilic medium, for (HH), we found just one species. The photophysical properties of all these species were determined, and we verified that each one of them displays distinct photophysical properties from one to another. For example, for monomer of (HN), the lowest electronic singlet state S₁ is (π,π^*) and the lowest electronic triplet state T₁ is (π,π^*), due to the phosphorescence lifetime it is t=0.8 s. For the (HH) monomer, the S₁ is (π,π^*) and T₁ is (π,π^*) and the spin–orbital coupling is inefficient. These determinations were used to characterise and to identify the harmane species that is solubilised into the interior of neutral (triton X-100), anionic (dodecyl lithium sulphate) and cationic (hexadecyltrimethyl ammonium bromide) micelles, all of them were prepared under physiological conditions. The results indicated that active species in the interior of the micelles is a hydrogen bond complex between (HN) and micellar environments that is anchored in the aqueous region of micelles.     

硝基甲烷光重排反应机理的从头算和组态相互作用的研究

硝基甲烷是最简单的硝基化合物,同时也是一种高能物质,在工业上有着重要的作用。对于硝基甲烷形成亚硝酸甲酯的光反应,不同的实验研究得到了不同的结论。     

Excitation-energy dependence of phosphorescence quantum yield of benzaldehyde vapour at low pressure

The phosphorescence quantum yield of benzaldehyde vapour was measured at low pressure (down to 2 mtorr) as a function of excitation wavelength. The quantum yield is essentially constant in the range of excitation energy corresponding to the S₁(n,π^*) state, but it decreases very rapidly as the excitation energy is raised to the value corresponding to S₂(π,π^*), indicating that the phosphorescence property of the benzaldehyde molecule varies, depending on the nature of the singlet state to which the molecule is initially excited.     

4-硝基咪唑A-带激发态结构动力学

通过共振拉曼光谱实验和量子化学计算的方法研究了4-硝基咪唑(4NI)A-带激发态衰变动力学.对4NI的振动光谱、紫外电子吸收光谱、荧光光谱和共振拉曼光谱进行了指认.在全活化空间自洽场法(CASSCF)/6-31G(d)计算水平下获得了单重激发态S1(nOπ*)和S2(ππ*)和势能面交叉点S1(nOπ*)/S2(ππ*)的优化几何结构和能量,分析了A-带共振拉曼光谱的强度模式特征,获得了短时结构动力学,并结合全活化空间自洽场法(CASSCF)理论计算结果确定了4NI在S2(ππ*)态衰变通道主要是S2,FC→S2,min(ππ*)→S0辐射弛豫.     

亚硝酸甲酯光解反应的从头算和Cl研究

用从头算和MP2方法求得亚硝酸甲酯的基态、第一和第二激发态解离为CH₃O和NO自由基的解离能分別为238.14、68.99和-183.97kJ/mol,而CH₃O和NO易于生成甲醛和硝酰。由CI方法求出的亚硝酸甲酯直接生成甲醛和硝酰的基态和激发态反应曲线表明,该反应难以按这种机理进行。因此,以上计算支持了实验提出的亚硝酸甲酯光反应生成甲醛和硝酰的两种机理中的光解离机制。     

Theoretical studies of electronic absorption and emission spectra of Pt(saloph)

The performance of ab initio calculations for the ground and excited states of the Pt(saloph) complex is examined in detail. The S₀–S_i and T₁–T_i absorption spectra are calculated, and the transition between the ground S₀ state and the excited S₁ state involves the HOMO-2, HOMO-1, HOMO and LUMO. Moreover, calculations show that the emissive singlet is of mixed MLCT/LLCT characteristic. On the other hand, the molecular geometry of the complex is nearly planar in the ground state while the geometry is obviously nonplanar in the excited state of S₁(π, π^*) in the gas phase.     

Low-lying excited singlet states and S2→S0 luminescence of dipyrido[3,4-b: 2,3-d]phenazine

The absorption, fluorescence and excitation fluorescence spectra dipyrido[3,4-b:2,3-d]-phenazine (DPPZ1) have been measured in non-polar and polar matrices at room temperature, and were taken into account to explain the origin of the relatively weak emission of this molecule in both type of environment. The electronic structure of DPPZ1 was calculated using a modified INDO CI method. The geometry optimization has been performed using the MNDO method. According to the spectra and the results of calculations, the lowest excited singlet state S₁ of DPPZ1 molecule is of n,π^*-type and the next one, S₂ state, is of π,π^*-type. The energy gap ΔE_calc is equal 4770 cm⁻¹. The low efficiency of the emission observed in the hydroxylic solvent can be interpreted in terms of thermal quenching of the π,π^*-type fluorescence. However, experimental results obtained suggest that in nonpolar solvents the emission of the molecule examined is an anomalous S₂→S₀ fluorescence.