[Ru(bpy)2(phen)]^2+主配体上双取代效应DFT法研究

对钌联吡啶菲咯啉配合物[Ru(bpy)2(phen)]^2+及其主配体(phen)上5,6-双取代衍生物,用密度泛函(DFT)法在B3LYP/LanL2DZ水平上进行理论计算研究。探讨供电子基团(OH)和拉电子基团(F)在主配体上的取代对配合物的电子结构及相关性质,如配合物前沿分子轨道的能量、组成、光谱性质、原子的净电荷布居及配位键长键角等的影响规律。计算结果表明,取代基对该系列取代衍生物的电子结构,特别是第一激发态的电子云分布影响较大,拉电子基团(F)能活化主配体,钝化辅助配体;而代电子基团(OH)则相反。无认是供电子基团(OH),还是拉电子基团(F)都导致取代衍生物的电子基谱带红移。此外,用基于极性交替规律及极性叠加概念的多系列箭头的图示方法对主配体上的原子净电荷布居的特征作了讨论。计算结果能较好地解释有关的实验现象与规律。     

Ru(bpy)32+配合物及bpy上双取代基效应的DFT法研究

报道Ru(bpy)32+配合物取代基效应的量子化学密度泛函(DFT)法研究的结果。探讨Ru(bpy)32+的三个配体bpy(2,2′-联二吡啶)被取代基(-NH2,-OH,-NO2)对位双取代后对配合物电子结构及相关性质,如配位键长、光谱性质等的影响规律,为该类配合物的合成及性质分析提供理论参考。     

M(bpy)_3~(2 )(M=Fe,Ru,Os)电子结构与相关性质

报导了对配合物M(bpy)2 M=Fe,Ru,Os)的量子化学密度泛函(DFT)法研究的结果.在B3LYP/LanL2DZ方法与基组的水平上进行计算 ,探讨M(bpy)32 的电子结构特征及相关性质 ,特别是中心原子对配合物的配位键长、光谱性质、电荷布居及化学稳定性等的影响规律 ,为该类配合物的合成 ,为分析光、电、催化作用机理提供理论参考.     

取代基效应对环金属Rh(Ⅲ)配合物二阶非线性光学性质影响的DFT研究

本文采用密度泛函理论(DFT)方法对系列环金属Rh(Ⅲ)配合物的结构与二阶非线性光学性质进行了计算研究.结果显示，配体中取代基的改变对配合物的几何结构和Wiberg键级影响不大.当主配体上的—H被其他强的供/吸电子基团取代时，配合物的极化率增大.其中，对于配合物1-6,主配体或副配体中强供/强吸电子基团的引入均有效地提高了配合物的第一超极化率(β_tot).而在配合物7-12中，配体中取代基的改变对配合物的β_tot值也有所提高，但幅度不大.此外，计算所得的配合物动态超瑞利散射超极化率(β_HRS)值与β_tot值的变化规律一致.对配合物的电子结构与吸收光谱的分析表明，体系具有较大的β_tot值与其吸收光谱的明显红移，较低的电子跃迁能，以及方向一致的电荷转移模式相关.     

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.     

三联吡啶Pt(Ⅱ)配合物的基态和激发态的理论研究

为了探究取代基对三联吡啶Pt(Ⅱ)配合物发光性质的影响, 采用MP2和CIS方法分别对配合物[Pt(trpy)C≡CC6H4R]+[trpy=2,2',6',2″-Terpyridine; R=NO2(1), Cl(2), H(3), CH3(4)]的基态和激发态的几何构型进行了优化, 通过TDDFT/B3LYP方法得到了这些化合物在二氯甲烷溶液中的磷光发射光谱以及它们的跃迁性质. 研究结果表明, 由于NO2的强吸引作用以及在C≡CC6H4NO2部分可能存在的电子共振结构, 化合物1的最低发射可以指认为Pt—C≡C→trpy(3MLCT/3LLCT) 的跃迁, 并且还有很大的一部分来自于π→π*(C6H4NO2) 跃迁的贡献, 而化合物3和化合物4由于含有给电子基团, 因此其最低发射仅仅是来自于3MLCT/3LLCT的跃迁. 但是并不是所有的取代基为吸电子基团时都能有类似的π→π*跃迁性质. 对于化合物2, Cl是仅次于NO2的吸电子取代基, 但是由于缺少电子共振的贡献, 它的跃迁性质却与化合物3和4相同. 另外, 激发态几何相对于基态几何没有发生太大的变化, 这与实验上所观察到的较小斯托克斯频移现象一致.     

M(bpy)2+3(M=Fe,Ru,Os)电子结构与相关性质

报导了对配合物(M=Fe,Ru,Os)的量子化学密度泛函(DFT)法研究的结果.在B3LYP/LanL2DZ方法与基组的水平上进行计算,探讨的电子结构特征及相关性质,特别是中心原子对配合物的配位键长、光谱性质、电荷布居及化学稳定性等的影响规律,为该类配合物的合成,为分析光、电、催化作用机理提供理论参考.     

铼联吡啶系列光敏染料的合成

铼联吡啶配合物具有较高的氧化-还原电位及较好的光热稳定性,吸收可见光后可形成强的MLCT过渡态(Metal-to-Ligand Charge Transfer Transition),而且铼联吡啶配合物具有特殊的平面结构,使得染料分子可以呈现更加规则的有序排列,使其在纳米二氧化钛表面吸附的数量增加,提高对太阳能的吸收利用率,可用作Gratzel太阳能电池的光敏剂,为了研究配体上取代基团对铼联吡啶配合物结构和性能的影响,本文合成了吡啶环上分别带有甲基、羟基、氨基等不同供电子基团的铼联吡啶系列配合物1a,1b,1c,1d。     

齐聚苯胺修饰的三联吡啶铁配合物的合成及其光谱和电化学性质

合成了一系列齐聚苯胺修饰的三联吡啶铁配合物,研究了齐聚苯胺链长、不同取代基等对配合物光谱性质和氧化还原性质的影响。 结果表明,相对于配合物[Fe(TPY)₂]²⁺(TPY:三联吡啶),供电子齐聚苯胺单元的引入,使得修饰基团与配合物中心核[Fe(TPY)₂]²⁺之间形成了强的D-A体系,导致配合物¹MLCT吸收波长显著红移至594 nm,且摩尔吸光系数增加近5倍。 配合物同时具有基于金属中心、三联吡啶配体和齐聚苯胺单元的多个氧化还原过程,强拉电子取代基使齐聚苯胺单元氧化还原峰简并且峰电势明显正移,而正丁基取代基对氧化还原峰电势的影响较小。     

镱(Ⅲ)卟啉配合物的合成、结构表征和近红外光谱研究

合成了5个meso-位和β-位具有不同取代基的Yb(Ⅲ)卟啉配合物(2a~2e), 并对其结构进行了表征; 研究了配合物的可见光谱和近红外光谱性质, 测得了相关的量子产率和荧光寿命. 研究结果表明, 此类中性单核Yb(Ⅲ)卟啉配合物由于Yb³⁺的存在, 导致卟啉配体发生π→π*跃迁, 并将吸收的可见光能量传递给Yb³⁺的激发态, 使得配合物在近红外光区有很强的发光, 且meso-位为供电子基团的Yb(Ⅲ)卟啉配合物的发光效率比含吸电子基团的Yb(Ⅲ)卟啉配合物高, 而β-位溴化的Yb(Ⅲ)卟啉配合物的发光效率较差.     

M(bpy)2+3(M=Fe,Ru,Os)电子结构与相关性质

报导了对配合物Ｍ（ｂｐｙ）＾２＋３（Ｍ＝Ｆｅ,Ｒｕ,Ｏｓ）的量子化学密度泛函法研究的结果。Ｂ３ＬＹＰ／ＬａｎＬ２ＤＺ方法与基组的水平上进行计算,探讨Ｍ（ｂｐｙ）＾２＋３电子结构特征及相关性质,特别是中心原子对配合物的配位键长、光谱性质,电荷布局及化学稳定性等的影响规律,为该类配合物的合成,为分析光、电、催化作用机理提供理论参考。     

Effect of intramolecular pi-pi and CH-pi interactions between ligands on structure, electrochemical and spectroscopic properties of fac-[Re(bpy)(CO)3(PR3)]+(bpy = 2,2'-bipyridine; PR3= trialkyl or triarylphosphines)

Intramolecular pi-pi and CH-pi interactions between the bpy and PR3 ligands of fac-[Re(bpy)(CO)3(PR3)]+ affect their structure, and electrochemical and spectroscopic properties. Intramolecular CH-pi interaction was observed between the alkyl groups on the phosphine ligand (R =nBu, Et) and the bpy ligand, and intramolecular pi-pi and CH-pi interactions were both observed between the aryl group(s) on the phosphorus ligand (R =p-MeOPh, p-MePh, Ph, p-FPh, OPh) and the bpy ligand, while no such interactions were found in the trialkylphosphite complexes (R = OiPr, OEt, OMe). The intramolecular interactions distort the pyridine rings of the bpy ligand as long as 3.7 x 10(-2)A in crystals. Molecular orbital calculations of the bpy ligand suggest that this distortion decreases the energy gap between its pi and pi* orbitals. An absorption band attributed to the pi-pi*(bpy) transition of the distorted rhenium complexes, measured in a KBr pellet, was red-shifted by 1-5 nm compared to the complexes without the distorted bpy ligand. Even in solution, similar red shifts of the pi-pi*(bpy) absorption were observed. The redox potential E1/2(bpy/bpy*-) of the complexes with the trialkylphosphine and triarylphosphine ligand are shifted positively by 110-120 mV and 60-80 mV respectively, compared with those derived from the electron-attracting property of the phosphorus ligand. In contrast with these properties, three nu(CO) IR bands, which are sensitive to the electron density on the central rhenium because of pi-back bonding, were shifted to higher energy, and a Re(I/II)-based oxidation wave was observed at a more positive potential according to the electron-attracting property of the phosphorus ligand.     

Syntheses, characterization, and photochemical properties of amidate-bridged Pt(bpy) dimers tethered to Ru(bpy)3(2+) derivatives

Amidate-bridged diplatinum(II) entities [Pt(2)(bpy)(2)(μ-amidato)(2)](2+) (amidate = pivalamidate and/or benzamidate; bpy = 2,2'-bipyridine) were covalently linked to one or two Ru(bpy)(3)(2+)-type derivatives. An amide group was introduced at the periphery of Ru(bpy)(3)(2+) derivatives to give metalloamide precursors [Ru(bpy)(2)(BnH)](2+) (abbreviated as RuBnH, n = 1 and 2), where deprotonation of amide BnH affords the corresponding amidate Bn, B1H = 4-(4-carbamoylphenyl)-2,2'-bipyridine, and B2H = ethyl 4'-[N-(4-carbamoylphenyl)carbamoyl]-2,2'-bipyridine-4-carboxylate. From a 1:1:1 reaction of [Pt(2)(bpy)(2)(μ-OH)(2)](NO(3))(2), RuBnH, and pivalamide, trinuclear complexes [Pt(2)(bpy)(2)(μ-RuBn)(μ-pivalamidato)](4+) (abbreviated as RuBn-Pt(2)) were isolated and characterized. Tetranuclear complexes [Pt(2)(bpy)(2)(μ-RuBn)(2)](6+) (abbreviated as (RuBn)(2)-Pt(2)) were separately prepared and characterized in detail. The quenching of the triplet excited state of the Ru(bpy)(3)(2+) derivative (i.e., Ru*(bpy)(3)(2+)) upon tethering the Pt(2)(bpy)(2)(μ-amidato)(2)(2+) moiety is strongly enhanced in RuB1-Pt(2) and (RuB1)(2)-Pt(2), while it is only slightly enhanced in RuB2-Pt(2) and (RuB2)(2)-Pt(2). These are partly explained by the driving forces for the electron transfer from the Ru*(bpy)(3)(2+) moiety to the Pt(2)(bpy)(2)(μ-amidato)(2)(2+) moiety (ΔG°(ET)); the ΔG°(ET) values for RuB1-Pt(2), (RuB1)(2)-Pt(2), RuB2-Pt(2), and (RuB2)(2)-Pt(2) are estimated as -0.01, 0.00, +0.22, and +0.28 eV, respectively. The considerable difference in the photochemical properties of the B1- and B2-bridged systems were further examined based on the emission decay and transient absorption measurements, which gave results consistent with the above conclusions.     

Electronic effect of different positions of the -NO2 group on the DNA-intercalator of chiral complexes [Ru(bpy)2L]2+ (L =o-npip, m-npip and p-npip)

New chiral Ru(II) complexes with intercalators L (L =o-npip, m-npip and p-npip) containing -NO2 at different positions on the phenyl ring were synthesized and characterized by elemental analysis, 1H NMR, ESI-MS and CD spectra. The DNA binding properties of these complexes have been investigated with UV-Vis, emission spectra, CD spectra and viscosity measurements. A subtle but detectable difference was observed in the interaction of these isomers with CT-DNA. Absorption spectroscopy experiments indicated that each of these complexes can interact with the DNA. The DNA-binding of the Delta-isomer is stronger than that of Lambda-isomer. DNA-viscosity experiments provided evidence that both Delta- and Lambda-[Ru(bpy)2(o-npip)](PF6)2 bind to DNA with partial intercalation, and both Delta- and Lambda-[Ru(bpy)(2)(p-npip)](PF6)2 fully intercalate with DNA. However, Delta- and Lambda- [Ru(bpy)2(m-npip)](PF6)2 bind to DNA through different modes, i.e., the Delta isomer by intercalation and Lambda isomer by partial intercalation. Under irradiation with UV light, Ru(II) complexes showed different efficiency of cleaving DNA. The most interesting feature is that neither 1 (Delta-1 and Lambda-1) nor 3 (Delta-3 and Lambda-3) emit luminescence either alone in aqueous solution or in the presence of DNA, whereas both Delta-2 and Lambda-2 emit luminescence under the same conditions. In addition, theoretical calculations for these three isomer complexes have been carried out applying the density functional theory (DFT) method at the level of the B3LYP/LanL2DZ basis set, and the calculated results can reasonably explain the obtained experimental trends in the DNA-binding affinities or binding constants (Kb) and some spectral properties of the complexes.     

Synthesis, characterization, and reactivity of [Ru(bpy)(CH3CN)3(NO2)]PF6, a synthon for [Ru(bpy)(L3)NO2] complexes

We report a high yield, two-step synthesis of fac-[Ru(bpy)(CH3CN)3NO2]PF6 from the known complex [(p-cym)Ru(bpy)Cl]PF6 (p-cym = eta(6)-p-cymene). [(p-cym)Ru(bpy)NO2]PF6 is prepared by reacting [(p-cymene)Ru(bpy)Cl]PF6 with AgNO3/KNO2 or AgNO2. The 15NO2 analogue is prepared using K15NO2. Displacement of p-cymene from [(p-cym)Ru(bpy)NO2]PF6 by acetonitrile gives [Ru(bpy)(CH3CN)3NO2]PF6. The new complexes [(p-cym)Ru(bpy)NO2]PF6 and fac-[Ru(bpy)(CH3CN)3NO2]PF6 have been fully characterized by 1H and 15N NMR, IR, elemental analysis, and single-crystal structure determination. Reaction of [Ru(bpy)(CH3CN)3NO2]PF6 with the appropriate ligands gives the new complexes [Ru(bpy)(Tp)NO2] (Tp = HB(pz)3-, pz = 1-pyrazolyl), [Ru(bpy)(Tpm)NO2]PF6 (Tpm = HC(pz)3), and the previously prepared [Ru(bpy)(trpy)NO2]PF6 (trpy = 2,2',6',2' '-terpyridine). Reaction of the nitro complexes with HPF6 gives the new nitrosyl complexes [Ru(bpy)TpNO][PF6]2 and [Ru(bpy)(Tpm)NO][PF6]3. All complexes were prepared with 15N-labeled nitro or nitrosyl groups. The nitro and nitrosyl complexes were characterized by 1H and 15N NMR and IR spectroscopy, elemental analysis, cyclic voltammetry, and single-crystal structure determination for [Ru(bpy)TpNO][PF6]2. For the nitro complexes, a linear correlation is observed between the nitro 15N NMR chemical shift and 1/nu(asym), where nu(asym) is the asymmetric stretching frequency of the nitro group.     

Aminoethylglycine-functionalized Ru(bpy)3(2+) with pendant bipyridines self-assemble multimetallic complexes by copper and zinc coordination

Directed self-assembly using inorganic coordination chemistry is an attractive approach for making functional supramolecular structures. In this article, the synthesis and characterization of Ru(bpy) 3 (2+) compounds derivatized with aminoethylglycine (aeg) substituents containing pendant bipyridine (bpy) ligands is presented. The free bpy ligands in these complexes are available for metal chelation to form coordinative cross-links; addition of Cu (2+) or Zn (2+) assembles heterometallic structures containing two or three transition-metal complexes. Control over relative placement of metal complexes is accomplished using two strategies: two bipyridine-containing aeg strands tethered to Ru(bpy) 3 (2+) allow intramolecular coordination and result in a dimetallic hairpin motif. Ru(bpy) 3 (2+) modified with a single strand forms intermolecular cross-links forming the trimetallic complex. Each of these is characterized by a range of methods, and their photophysical properties are compared. These data, and comparison to an acetyl aeg- modified Ru(bpy) 3 (2+) complex, confirm that the metal ions cross-link bpy-containing aeg strands. Heterometallic complexes containing bound Cu (2+) cause a dramatic reduction in the Ru(bpy) 3 (2+) quantum yields and lifetimes. In contrast, the Ru(bpy) 3 (2+) hairpin with coordinated Zn (2+) has only a slight decrease in quantum yield but no change in lifetime, which could be a result of steric impacts on structure in the dimetallic species. Analogous effects are not observed in the trimetallic Ru-Zn-Ru structures in which this constraint is absent. Each of these heterometallic structures represents a facile and reconfigurable means to construct multimetallic structures by metal-coordination-based self-assembly of modular artificial peptide units.     

Synthesis,Characterization, Electrochemical and Spectroscopic Properties of [Ru(dppt)(bpy)Cl]+ and [Ru(pta)(bpy)Cl]+

Two novel Ru^II complexes [Ru(dppt)(bpy)Cl]ClO₄ (1) and [Ru(pta)(bpy)Cl]ClO₄ (2)[dppt, pta and bpy = 3-(1,10-phenanthrolin-2-yl)-5,6-diphenyl-as-triazine, 3-(1,10-phenanthrolin-2-yl)-as-triazino[5,6-f]acenaphthylene and 2,2-bipyridine, respectively] were synthesized and characterized by elemental analysis and electrospray mass spectrometry, ¹H-n.m.r., and u.v.–vis spectroscopy. The redox properties of the complexes were examined using cyclic voltammetry. Due to the strong -accepting character of asymmetric ligands, the MLCT bands of (1) and (2) are shifted significantly to lower energies by comparison with [Ru(tpy)(bpy)Cl]⁺.