两种Zn(Ⅱ)配合物电子结构和光谱性质的理论研究

为了探究Zn(Ⅱ)配合物Zn(ATSM)(A)和Zn(BTSC)(DMSO)(B)的电子结构和光谱性质,采用M06方法优化了它们的基态几何构型,并利用计算得到的电子结构信息绘制了配合物在吸收过程中的电子云分布图.理论模拟出的吸收光谱数据与实验结果吻合较好.而且,在理论上检测到了实验上没有报道到的吸收峰.     

用密度泛函理论研究两种金属镍席夫碱配合物的电子结构和光谱性质

采用密度泛函理论(DFT),在B3LYP/6-31+G(d)-LANL2DZ水平上,研究了两种Ni(II)的席夫碱配合物1和2基态的几何结构,并在相同水平上进行了频率分析以确认稳定点的性质.基于优化的几何构型,在TDB3LYP/6-31+G(d)-LANL2DZ水平上,采用极化连续介质模型(PCM)在N,N-二甲基甲酰胺溶液中计算了配合物1和2的电子结构和紫外吸收光谱.结果显示,当配体对位上的Br原子被-NO2取代时,配合物的HOMO-LUMO能级差增大,从而导致配合物2的最大吸收波长相对于配合物1的发生蓝移.     

两种8-羟基喹啉锌配合物电子结构和光谱性质的理论研究

采用密度泛函理论在PBE0/6-31+G(d)-LANL2DZ水平下优化了两种8-羟基喹啉锌配合物的基态几何构型,并在相同水平下进行了频率分析以确认稳定点的性质.根据基态优化的构型,在TD-PBE0/6-31+G(d)-LANL2DZ水平下,采用极化连续介质模型(PCM)计算了甲醇溶剂中配合物的电子结构和电子吸收光谱.计算结果表明,配合物B中8-羟基喹啉2号位取代基蒽较大的π共轭作用使其具有较小的HOMO-LUMO能级差,从而使配合物B的最大吸收波长发生了红移现象.     

二硫代氨基甲酸盐过渡金属配合物的合成及三阶非线性光学性质研究

以对苯二胺为原料合成了二硫代氨基甲酸盐过渡金属［Ｎｉ（Ⅱ）,Ｐｄ（Ⅱ）,Ｐｒ（Ⅱ）］配合物及其它相应脱质子产物卡宾二硫代胺基甲酸盐配合物．通过元素分析,ＩＲ,ＵＶ测试表征．对该系列配合物用四波混频方法,研究了它们的三阶非线性光学性质．结果表明,平面型二硫代甲酸盐配合物有较强的三阶非线性光学效应．并且它们脱去质子形成的配合物共轭体系更大,其三阶非线性光学效应明显提高．     

三种席夫碱-Ni(Ⅱ)配合物的电子结构和吸收光谱的理论计算

采用B3LYP/6-31+G(d)-LANL2DZ方法优化了三种Ni(Ⅱ)的席夫碱配合物基态的几何构型,并在相同水平下进行了频率分析以确认稳定点的性质;利用含时密度泛函理论和极化连续介质模型(PCM),按TDB3LYP/6-31+G(d)-LANL2DZ水平计算了目标配合物在N,N-二甲基甲酰胺溶剂中的电子结构和吸收光谱.计算结果表明,配体中间位甲氧基的存在使配合物A具有较大的HOMO-LUMO能级差;且三种Ni(Ⅱ)配合物的S0→S1态的跃迁能按照A→B→C的顺序依次降低.     

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.     

8-羟基喹啉锰配合物电子结构和光谱性质的含时密度泛函研究

采用密度泛函理论(DFT)B3LYP方法, 对8-羟基喹啉锰配合物进行结构优化, 探讨了配合物的结构、分子轨道能级和组成、电荷分布和转移等; 采用含时密度泛函理论(TDDFT)B3LYP/6-31G(d,p)方法对配合物的电子结构进行计算, 获得其吸收光谱. 结果表明, Mn(Ⅲ)与8-羟基喹啉中的N原子和O原子形成不对称六配位的稳定配合物, 金属锰对前线轨道的贡献很大, 在HOMO轨道中占28.53%, 在LUMO轨道中占68.30%; 中心金属锰(Ⅲ)强烈地参与发光, 电子在基态与激发态之间的跃迁, 主要是中心金属锰及8-羟基喹啉配体间的电荷转移, 在可见光区存在2个强度较大的吸收峰, 分别位于756.8 nm和532.7 nm处. 通过对双分子体系的研究发现, 相邻2个分子之间能够进行微量电荷的转移, 分子间的相互作用对前线轨道组成有明显的影响.     

N，N-二甲酰基二硫代氨基甲酸根金属配合物的研究

本文首次报道了一系列N，N-二甲酰基二硫代氨基甲酸根为配体的过渡金属配合物，对它们进行了化学分析、光谱表征和磁性质研究。研究结果表明，在配合物中，配体二硫代氨基甲酸根一般为较弱的双齿配位。     

联吡啶Ir(Ⅲ)配合物电子结构及光谱性质的理论研究

采用密度泛函理论(DFT)对配合物Ir(ppy)2(N^N)+ [ppy=2-phenylpyrine, N^N=bpy= 2,2’-bipyridine(1); N^N=H2dcbpy=4.4’-dicarboxy-2,2’-bipyridine(2), N^N=Hcmbpy=4-carboxy-4’-methyl-2,2’-bipyridine(3)] 的基态和激发态几何构型进行优化, 通过TDDFT/B3LYP方法得到这些化合物在乙腈溶液中的吸收光谱和磷光发射光谱及其跃迁性质. 研究结果表明, 化合物1 (384 nm), 2(433 nm)和3 (413 nm) 最低的吸收谱被指认为MLCT/LLCT[dIr+π(ppy)→π*(N^N)]电荷跃迁. 化合物1(486 nm), 2(576 nm)和3 (567 nm)最低的磷光发射可以描述为[dIr+π(ppy)]→[π*(N^N)]跃迁. 这是由于联吡啶配体上吸电子基团的引入, 稳定了相应的空轨道, 导致了化合物2和3的吸收和发射光谱红移. 同时, 化合物非线性光学性质的计算结果表明, 三种化合物均具有较大的一阶超极化率(β), 联吡啶配体中吸电子基团的增加, 使得分子内电子转移增强, 导致一阶超极化率增大.     

一类新型苯基吡唑铱(Ⅲ)配合物的电子结构及光谱性质

为了探索新型苯基吡唑铱(Ⅲ)配合物的电子结构与光谱性质之间的关系,采用密度泛函理论(DFT)优化了铱金属配合物(ppz)2Ir(BTZ)(1)和(ppz)2Ir(4-TfmBTZ)(2)的基态与激发态的几何结构.通过含时密度泛函理论(TD-DFT)方法计算了配合物的吸收和发射谱,指认了它们的跃迁性质.和Ir(ppz)3相比,通过引入新的辅助配体并对其修饰实现了发光颜色的调节.配合物1和2的最低能磷光发射可指认为3MLCT/3LLCT/3ILCT[π*(R-BTZ)→d(Ir)+π(ppz)+π(R-BTZ)]的电荷混合跃迁.此外,它们的磷光发射和吸收有相似的跃迁性质.MLCT主要发生在Ir(R-BTZ)片段而不是Ir(ppz)2片段.第二配体在此配合物的发光过程中起了主要作用.     

Theoretical study on electronic structures,spectra, and charge transporting properties of two Pt(II) complexes with triazenido ligands

Russian Journal of General Chemistry - Two compounds 1-[(2-carboxymethyl)benzene]-3-[2-pyridine]triazene (HL) and 1-[(2-carboxymethyl) benzene]-3-[o-aminobenzoic acid]triazene (H2L') and two...     

EPR and electronic spectral properties of aryl-substituted bis(dithiophosphato)copper(II) complexes

The spectral properties of bis(diaryl-dithiophosphato)copper(II) complexes, [Cu(S(2)P(OR)(2))(2)], with R = o-cresyl (complex I) and 2,6-dimethylphenyl (complex II) are studied by EPR- and vis spectroscopy. In solid (powder) state both complexes exhibit dark brown colour and are paramagnetic. Room temperature EPR spectra of the complexes dissolved in non-coordinating (C(6)H(5)CH(3), C(5)H(12), C(6)H(14)), acceptor (CHCl(3), CCl(4)) or donor (DMFA, DMSO) solvents have typical features of the chromophore CuS(4). In non-coordinating and acceptor solvents their isotropic EPR parameters are: g(iso)=2.047+/-0.003, (Cu)A(iso) = 7.2+/-0.1 mT and (P)A = 0.95+/-0.1 mT. An absorption band characterizes the vis spectra in these solvents with a maximum at 427 nm, due to a ligand-to-metal charge-transfer transition. One hour after dissolution the absorbance at 427 nm follows Beer's law with molar absorptivity (epsilon) about 11000, which does not change significantly after 24 h staying at room temperature or after 30 min heating at 50 degrees C. Both DMFA and DMSO exhibit specific solute-solvent interaction with the acceptor centre of copper complex yielding an axial adduct, with increased g-factor and decreased (hf)A compared to the initial complex. An additional EPR signal with unresolved hyperfine structure is also detected in DMSO. EPR and vis intensities of both bis(diaryl-dtp)Cu(II) complexes decrease after dissolution in both solvents. Moreover, they are EPR silent in pyridine and do not show any absorption in the vis spectra.     

Syntheses and electronic structures of one-electron-oxidized group 10 metal(II)-(disalicylidene)diamine complexes (metal = Ni, Pd, Pt)

Group 10 metal(II) complexes of H2tbu-salen (H2tbu-salen = N,N'-bis(3',5'-di-tert-butylsalicylidene)ethylenediamine) and H2tbu-salcn (H2tbu-salcn = N,N'-bis(3',5'-di-tert-butylsalicylidene)-1,2-cyclohexanediamine) containing two 2,4-di(tert-butyl)phenol moieties, [Ni(tbu-salen)] (1a), [Ni(tbu-salcn)] (1b), [Pd(tbu-salen)] (2a), [Pd(tbu-salcn)] (2b), and [Pt(tbu-salen)] (3), were prepared and structurally characterized by X-ray diffraction, and the electronic structures of their one-electron-oxidized species were established by spectroscopic and electrochemical methods. All the complexes have a mononuclear structure with two phenolate oxygens coordinated in a very similar square-planar geometry. These complexes exhibited similar absorption spectra in CH2Cl2, indicating that they all have a similar structure in solution. Cyclic voltammograms of the complexes showed a quasi-reversible redox wave at E1/2 = 0.82-1.05 V (vs Ag/AgCl), corresponding to formation of the relatively stable one-electron-oxidized species. The electrochemically oxidized or Ce(IV)-oxidized species of 1a, 2a, and 3 displayed a first-order decay with a half-life of 83, 20, and 148 min at -20 degrees C, respectively. Ni(II) complexes 1a and 1b were converted to the phenoxyl radicals upon one-electron oxidation in CH2Cl2 above -80 degrees C and to the Ni(III)-phenolate species below -120 degrees C. The temperature-dependent conversion was reversible with the Ni(III)-phenolate ground state and was found to be a valence tautomerism governed by the solvent. One-electron-oxidized 1b was isolated as [Ni(tbu-salcn)]NO3 (4) having the Ni(II)-phenoxyl radical ground state. One-electron-oxidized species of the Pd(II) complexes 2a and 2b were different from those of the Ni(II) complexes, the Pd(II)-phenoxyl radical species being the ground state in CH2Cl2 in the range 5-300 K. The one-electron-oxidized form of 2b, [Pd(tbu-salcn)]NO3 (5), which was isolated as a dark green powder, was found to be a Pd(II)-phenoxyl radical complex. On the other hand, the ESR spectrum of the one-electron-oxidized species of Pt(II) complex 3 exhibited a temperature-independent large g anisotropy in CH2Cl2 below -80 degrees C, while its resonance Raman spectrum at -60 degrees C displayed nu8a of the phenoxyl radical band at 1600 cm-1. These results indicated that the ground state of the Pt(II)-phenoxyl radical species has a large distribution of the radical electron spin at the Pt center. One-electron oxidation of 3 gave [Pt(tbu-salen)]NO3 (6) as a solid, where the oxidation state of the Pt center was determined to be ca. +2.5 from the XPS and XANES measurements.     

DFT/TDDFT studies on the electronic structures and spectral properties of rhenium(I) pyridinybenzoimidazole complexes

The electronic structures and spectral properties of three Re(I) complexes [Re(CO)3XL] (X = Br, Cl; L = 1-(4-5'-phenyl-1,3,4-oxadiazolylbenzyl)-2-pyridinylbenzoimidazole (1), 1-(4-carbazolylbutyl)-2-pyridinylbenzoimidazole (2), and 2-(1-ethylbenzimidazol-2-yl)pyridine (3)) were investigated theoretically. The ground and the lowest lying triplet excited states were fully optimized at the B3LYP/LANL2DZ and CIS/LANL2DZ levels, respectively. TDDFT/PCM calculations have been employed to predict the absorption and emission spectra starting from the ground and excited state geometries, respectively. The lowest lying absorptions were calculated to be at 481, 493, and 486 nm for 1-3, respectively, and all have the transition configuration of HOMO-->LUMO. The lowest lying transitions can be assigned as metal/ligand-to-ligand charge transfer (MLCT/LLCT) character for 1, ligand-to-ligand charge transfer (LLCT) character for 2, and mixed MLCT/LLCT and intraligand pi-->pi* charge transfer (ILCT) character for 3. The emission of 1 at 551 nm has the MLCT/(3)LLCT character, 2 has the (3)MLCT/(3)LLCT character at 675 nm, and the 651 nm transition of 3 has the character of (3)MLCT/(3)LLCT/(3)ILCT. Ionization potentials (IP) and electron affinities (EA) calculations show that the comparable EA and smaller IP values and the relatively balanceable charges transfer ability of 2 with respect to 1 and 3 result in the higher efficiency of OLEDs. The calculated results show that the absorption and emission transition character and device's efficiency can be changed by altering the ancillary ligands.     

(P-Bis(pentafluorophenyl) substituted) PCP-pincer Ru(II) complexes: A theoretical study of the molecular structure and electronic properties

The differences between the molecular structures of the PCP-pincer complex [RuCl{C₆H₃(CH₂P(C₆H₅)₂)₂-2,6}(PPh₃)] ([RuCl(PCP^H)(PPh₃)], 1) and its tetrakis-pentafluorophenyl substituted analogue [RuCl{C₆H₃(CH₂P(C₆F₅)₂)₂-2,6}(PPh₃)] ([RuCl(PCP^F20)(PPh₃)], 2) have been rationalised by performing calculations on the cations [Ru(PCP^H)(PPh₃)]⁺ (1cat) and [Ru(PCP^F20)(PPh₃)]⁺ (2cat). The molecular interactions between the chloride ligand and the axial rings, as found in 1 and 2, respectively, have been studied computationally in the model systems [(C₆X₅PH₂)₂Cl⁻] (X = H, F). The calculations on 2cat show that in 2 it is most likely the attractive electrostatic interaction between the chloride ligand and the fluorinated phenyl rings that forces the C_ipso atom to occupy an axial position rather than an equatorial one in the observed (X-ray of 2) square pyramidal arrangement. In 1, however, repulsive steric hindrance forces the PPh₃ ligand to take the apical position. The applicability of the TD-DFT method for the calculation of the electronic spectra of the PCP-pincer compounds 1 and 2 has been tested. The results indicate that the excitation energies calculated for both complexes are in a reasonable agreement with the experimental absorption maxima. However, for 1, all the calculated transition energies are underestimated.     

A theoretical study on the electronic structures and equilibrium constants evaluation of Deferasirox iron complexes

Elemental iron is essential for cellular growth and homeostasis but it is potentially toxic to the cells and tissues. Excess iron can contribute in tumor initiation and tumor growth. Obviously, in iron overload issues using an iron chelator in order to reduce iron concentration seems to be vital. This study presents the density functional theory calculations of the electronic structure and equilibrium constant for iron-deferasirox (Fe-DFX) complexes in the gas phase, water and DMSO. A comprehensive study was performed to investigate the Deferasirox-iron complexes in chelation therapy. Calculation was performed in CAMB3LYP/6-31G(d,p) to get the optimized structures for iron complexes in high and low spin states. Natural bond orbital and quantum theory of atoms in molecules analyses was carried out with B3LYP/6-311G(d,p) to understand the nature of complex bond character and electronic transition in complexes. Electrostatic potential effects on the complexes were evaluated using the CHelpG calculations. The results indicated that higher affinity for Fe(III) is not strictly a function of bond length but also the degree of Fe–X (X = O,N) covalent bonding. Based on the quantum reactivity parameters which have been investigated here, it is possible reasonable design of the new chelators to improve the chelator abilities.     

Molecular and electronic structures of one-electron oxidized Ni(II)-(dithiosalicylidenediamine) complexes: Ni(III)-thiolate versus Ni(II)-thiyl radical states

The dithiosalicylidenediamine Ni II complexes [Ni(L)] (R=tBu, R'=CH2C(CH3)2CH2 1, R'=C6H4 2; R=H, R'=CH2C(CH3)2CH2 3, R'=C6H4 4) have been prepared by transmetallation of the tetrahedral complexes [Zn(L)] (R=tBu, R'=CH2C(CH3)2CH2 7, R'=C6H4 8; R=H, R'=CH2C(CH3)2CH2 9, R'=C6H4 10) formed by condensation of 2,4-di-R-thiosalicylaldehyde with diamines H2N-R'-NH2 in the presence of Zn II salts. The diamagnetic mononuclear complexes [Ni(L)] show a distorted square-planar N2S2 coordination environment and have been characterized by 1H- and 13C NMR and UV/Vis spectroscopies and by single-crystal X-ray crystallography. Cyclic voltammetry and coulombic measurements have established that complexes 1 and 2, incorporating tBu functionalities on the thiophenolate ligands, undergo reversible one-electron oxidation processes, whereas the analogous redox processes for complexes 3 and 4 are not reversible. The one-electron oxidized species, 1+ and 2+, can be generated quantitatively either electrochemically or chemically with 70 % HClO4. EPR and UV/Vis spectroscopic studies and supporting DFT calculations suggest that the SOMOs of 1+ and 2+ possess thiyl radical character, whereas those of 1(py)2 + and 2(py)2 + possess formal Ni III centers. Species 2+ dimerizes at low temperature, and an X-ray crystallographic determination of the dimer [(2)2](ClO4)2.2 CH2Cl2 confirms that this dimerization involves the formation of a S-S bond (S...S=2.202(5) A).