H2S键合金属(II)咪唑卟啉配合物的结构、光谱和反应活性

选取8个典型的二价金属咪唑卟啉MP(M=Ca, Mg, Zn, Cu, Ni, Fe, Co, Mn; P代表咪唑卟啉)与H₂S(L)形成轴向金属配合物(L-MP; L-MP^*-L, P^*代表卟啉), 应用轨道和自旋概念密度泛函工具, 在优化构型的基础上, 通过自然键轨道(NBO)方法和前线轨道能级研究了它们的分子结构、光谱性质和反应活性. 模拟结果揭示L-MP和L-MP^*-L结构、光谱及其反应活性不同于其前体MP. MP排斥钙而选择镁; L对MP的结构影响较少, 与咪唑铁卟啉(FeP)能形成最稳定的单轴配合物(L-FeP), 其电子吸收光谱较前体FeP有显著的变化; 铁的亲核Fukui轨道指数值(f_Fe⁺)大于其他原子的Fukui指数, 且发生符号改变. 铁体系的自旋极化Fukui密度图也支持以上结论. 在这些典型的赤道键合配合物中, 金属M与N(S)原子之间的二级微扰相互作用能、自然电荷以及概念密度泛函指数等存在一系列线性关系. 以上结果可为理解内源性H₂S与血管性物质的相互作用机理提供启示.     

三聚氰胺金属(Ⅱ)配合物的结构、紫外-可见光谱和反应活性

三聚氰胺是婴幼儿"肾结石事件"的重要前体.本文选取几个典型的二价金属离子与三聚氰胺(L)形成的三聚氰胺金属配合物ML2(OH)2(M=Ca,Mg,Zn,Cu,Ni,Fe),使用密度泛函理论(DFT)、含时DFF和概念DFT等工具,系统地计算和比较了ML2(OH)2的结构、紫外-可见光谱和反应性质的异同.模拟结果揭示了ML2(OH)2的结构、光谱及其反应性质是一类不同于其前体L,形成ML2(OH)2配合物后,将有较高的亲电指数和较低的化学硬度以及呈现红外吸收峰红移;在这些典型的二价金属配合物中,金属M离子电荷与配体O和N原子之间的电荷、以及与金属M离子和配体原子之间的二级微扰相互作用能,配合物最低空轨道能级与其亲电反应指数、最低空轨道能级与化学硬度指数等方面,存在着一系列定量的相关关系,相关系数(R2)达0.889-0.997;前线分子轨道模拟结果表明,ML2(OH)2体系反应活性的差异源于金属离子对前线轨道贡献有所不同,FeL2(OH)2、CuL2(OH)2、NiL2(OH)2等过渡金属离子的配合物中,金属离子贡献较多,共价性成分较多.这些结果将为进一步理解人体内三聚氰胺致结石的成因提供有益的启示.     

三聚氰胺金属(II)配合物的结构、紫外-可见光谱和反应活性

三聚氰胺是婴幼儿“肾结石事件”的重要前体. 本文选取几个典型的二价金属离子与三聚氰胺(L)形成的三聚氰胺金属配合物ML2(OH)2(M=Ca, Mg, Zn, Cu, Ni, Fe), 使用密度泛函理论(DFT)、含时DFT和概念DFT等工具, 系统地计算和比较了ML2(OH)2的结构、紫外-可见光谱和反应性质的异同. 模拟结果揭示了ML2(OH)2的结构、光谱及其反应性质是一类不同于其前体L, 形成ML2(OH)2配合物后, 将有较高的亲电指数和较低的化学硬度以及呈现红外吸收峰红移; 在这些典型的二价金属配合物中, 金属M离子电荷与配体O和N原子之间的电荷、以及与金属M离子和配体原子之间的二级微扰相互作用能, 配合物最低空轨道能级与其亲电反应指数、最低空轨道能级与化学硬度指数等方面, 存在着一系列定量的相关关系, 相关系数(R2)达0.889-0.997; 前线分子轨道模拟结果表明, ML2(OH)2体系反应活性的差异源于金属离子对前线轨道贡献有所不同, FeL2(OH)2、CuL2(OH)2、NiL2(OH)2等过渡金属离子的配合物中, 金属离子贡献较多, 共价性成分较多. 这些结果将为进一步理解人体内三聚氰胺致结石的成因提供有益的启示.     

苯并咪唑羧酸及其碱土金属配合物电子光谱性质的含时密度泛函及其概念密度泛函研究

用密度泛函理论(DFT)以及B3 LYlP泛函在6-311++G**水平上,对苯并咪唑羧酸(L)及其3种碱土金属配合物ML(M=Mg,Ca,Ba)的基态(S0)结构进行优化,用含时密度泛函理论(TD-DFT)在6-311++G**水平下计算其吸收光谱.用单激发组态相互作用(CIS)法在HF/6-31+G*上优化其最低激发单重态(S1)的几何结构,用ID-DFT B3IYP/6-311++G**计算其发射光谱.结果表明,配体L与M(Ⅱ)结合成ML后,随原子序数的增大(Mg相似文献   

19电子配合物非线型M—C—O本质的密度泛函研究(M=Fe,Ru,Os)

采用密度泛函理论方法,对一系列19电子铁族配位化合物CpM(CO)2L·进行了结构优化和能量计算.计算结果表明:配体L为羰基时,同族三金属Fe,Ru和Os配合物中都会出现一个弯曲的M—C—O,金属M的电子转移到CO上以满足18电子规则的特征;当L为磷配体时,Fe配合物中2个M—C—O都是线型的.而Ru和Os两者表现类似,可以存在2种不同的结构:第1种是2个M—C—O都是线型的;第2种是有一个线型M—C—O,而另一个M—C—O是弯曲的.理论计算得到的弯曲结构更稳定的结果和实验相符.配合物几何结构的差异可以通过三金属原子的电子构型、原子半径和电子转移得到解释.     

异亚硝基乙酰乙酸乙酯亚胺Pd(Ⅱ)配合物的合成、表征和tran Pd(p-CH3C6H4-IEAI)2的晶体结构

二齿异亚硝基-β-酮胺配体,由于异亚硝基(肟基)配位功能引起人们的兴趣.在已知的这类配体的金属配合物中,肟基可通过N原子或/和O原子与金属原子配位形成各种键合异构体[1-4].     

活性钌、锇-配体多重键配合物研究进展

金属一配体多重键配合物的反应性研究有助人们深入理解许多重要的金属催化过程,如生物体系中的氧化和固氮及有机合成中的金属催化原子或基团转移反应．含Os=N多重键的锇（VI）氮合物在还原剂存在下发生氮偶合反应生成双核氮分子桥连配合物,为与固氮机理有关的金属氮合物氮偶合反应提供实验证据．一系列具有可调结构和氧化性含M=O,M=NR,M=CR^1R^2（M=Ru,Os）多重键的活性钌／锇氧合物,钌亚胺基配合物,钌／锇卡宾配合物（包括手性配合物）已被成功分离,其结构已通过光谱手段和x射线单晶衍射确定．这些活性金属一配体多重键配合物分别能与有机化合物发生氧原子、亚胺基、卡宾转移反应,包括烯烃环氧化、环氮化、环丙烷化、cis双羟基化,c—H键羟基化、酰胺化、卡宾插入等,从而允许直接研究相应催化过程中金属．配体多重键中间体的原子或基团转移反应,为金属催化原子或基团转移反应（包括不对称催化反应）提供重要机理信息．已发展出一系列涉及钌．配体多重键活性物种的高选择性钌催化反应,包括2,6-Cl2pyNO与烯烃的环氧化和Wacker型氧化成醛,H2O2水溶液氧化烯、炔烃和醇为羧酸或cis-二醇,PhI=NR与饱和c—H键的酰胺化,重氮化合物的卡宾偶合,分子内卡宾插入c—H键,重氮化合物、亚胺、烯／炔烃的三组分偶合,及以“PhI（OAc）2＋RNH2”为氮源的金属催化C—N键形成反应等．     

界面缩聚法合成聚卟啉金属配合物及其表征

利用对苯二甲酰氯交联meso-5,10,15,20一四（对羟基苯基）卟啉单体制备了聚卟啉配体及其Co（Ⅱ）、Mn（II）和Zn（Ⅱ）金属配合物,并对聚卟啉配体和金属配合物进行了红外光谱、扫描电镜和X射线光电子能谱分析。结果表明,卟啉单体是典型的晶体结构,而发生界面聚合过程中以平面二维方式进行,形成膜状聚合物;当金属离子与卟啉形成配合物后,其中一对N—H键中质子被配位金属取代,N1s轨道的电子结合能变化小于0．2eV,环中另外两个N原子与配位金属形成σ配位键,导致配位金属M2p3／2的电子结合能变化大于0．5eV,引起了卟啉环内层电子密度的变化。     

含有Pt―Pt键金属配合物的电子结构和二阶非线性光学性质

采用量子化学密度泛函理论(DFT)结合有限场(FF)的方法对一系列含有Pt―Pt键金属配合物的电子结构和二阶非线性光学(NLO)性质进行了理论计算. 结果表明改变共轭配体对Pt―Pt键影响不大. 由配体到Pt―Pt金属基团的电荷转移强度随配体增长而变大. 金属配合物静态一阶超极化率随配体的增长而增大, 配合物电荷的改变基本不影响这类化合物的二阶NLO性质. 具有相对长的共轭配体的配合物IId具有最大的二阶NLO响应. 含时密度泛函理论(TD-DFT)计算表明配合物IId的二阶NLO响应来自于混有配体到金属的配体内的π→π^*电荷转移跃迁的贡献.     

具有三维结构的Co(II)配合物二阶非线性光学性质的DFT研究

以实验合成出的Schiff碱配体和Co(II)配合物为母体,设计了Schiff碱配体和具有三维结构的Co(II)配合物.采用密度泛函理论的B3LYP/6-31g(d)-FF方法对具有开壳层电子组态Co(II)配合物及相应配体的二阶非线性光学(NLO)效应进行了计算.结果表明:Schiff碱配体形成配合物后分子的二阶NLO性质没有发生大的改变,这是由于金属Co2 离子在配合物电荷转移(CT)过程中起到了桥的作用,对分子的二阶NLO响应直接贡献不大.结合配合物的前线分子轨道分析发现,在分子内电荷转移过程中,对分子二阶NLO系数的主要贡献是配体内电荷转移(ILCT)跃迁.     

Experimental and density functional theory insights into the effect of withdrawing ligands on the fluorescence yield of Ru(II)‐based complexes

The quality of emission spectra of metal complexes gives good insights into their performance in many optoelectronic applications. Herein, the effect of the number and position of various ligand structures on the emission spectra of Ru bipyridine complexes was studied. Specifically, the use of a different number of withdrawing groups (COOH) was investigated in detail. The complexes were first investigated using density functional theory (DFT) and time‐dependent DFT calculations and then confirmed experimentally. The bandgap energy, reactivity, emission spectra and Stokes shift were found to depend on the number and position of the withdrawing groups attached to the Ru(bpy)₂²⁺ complexes. Upon increasing the number of withdrawing groups, the electrons were found to be withdrawn from the carbon orbitals and resonated to reach the metal, and accumulated around it, thus enhancing the metal‐to‐ligand charge transfer mechanism instead of the ligand‐to‐ligand charge transfer mechanism. The complexes with more withdrawing groups showed spectra with more intense emission peaks with shorter lifetime, indicating the enhancement in the photoactivity of the complexes. Ligands with ring nitrogens with two COOH groups showed the greatest effect on the enhancement of the emission spectra with a lifetime of 0.5359 ns. The resulting collective emission spectra covered a wide wavelength range, making the investigated complexes a good choice for many optoelectronic applications.     

羰基镍簇Ni(CO)n(n=1-4)的结构和Ni-CO键解离性质的密度泛函理论研究

在密度泛函理论框架下, 应用不同泛函计算了配合物Ni(CO)n(n=1~4)的平衡几何构型和振动频率. 考察了泛函和基组重叠误差对预测Ni—CO键解离能的影响. 计算结果表明, 用杂化泛函能得到与实验一致的优化几何构型和较合理的振动频率. 对Ni(CO)n(n=2~4)体系, 用“纯”泛函, 如BP86和BPW91, 可得到与CCSD(T)更符合、 并与实验值接近的解离能. 当解离产物出现单个金属原子或离子(如金属羰基配合物的完全解离)时, BSSE校正项的计算中应保持金属部分的电子结构一致. 只有考虑配体基组和不考虑配体基组两种情况下金属的电子构型与配合物中金属的构型一致时, 才能得到合理的BSSE校正, 从而预测合理的解离能.     

A comparative DFT study of some N-based aromatic ligand metal complexes as anticancer agents and analysis of their mode of interaction with DNA base pair

Metal complexed anticancer agents interact with DNA nucleobase pairs (AT and GC) through different types of binding mode such as intercalation, groove binding, covalent binding, etc. Minor and major groove binding mechanism of DNA base pair is the key factor for all kinds of anticancer agent; as metal complexes have a great affinity to bind with DNA nucleobase either through minor or major groove. Ligands in metal complexes also play a vital role during the interaction with DNA base pairs; these ligands directly interact with DNA through different interacting modes. Generally, anticancer agents with less sterically hindered N-based aromatic and planar ligands are the key component for DNA binding; as the structure of such ligands are quite compatible for following intercalation and groove binding mechanism. Since, the experimental investigation for drug-DNA nucleobase complexes are extremely complicated, therefore; quantum mechanical calculations might be very helpful for computing the actual interactions in drug-DNA complexes. Quantum mechanical approaches such as density functional theory (DFT) might be a very important and useful tool to investigate the actual mode of interaction of metal complexed antitumor agents with DNA nucleobase. Herein, we have taken some metal complexes with N-based aromatic ligands as antitumor agents to investigate the proper mode of interaction between drug-DNA complexes.     

Accurate Structure and Bonding Description of the Transition Metal‐Disulfur Monoxide Complexes [(PMe3)2M(S2O)] (M = Ni,Pd, Pt): Grimme Dispersion Corrected DFT Study

Geometry and bonding energy analysis of M–S₂O bonds in the metal‐disulfur monoxide complexes [(PMe₃)₂M(S₂O)] of nickel, palladium, and platinum were investigated at DFT, DFT‐D3, and DFT‐D3(BJ) methods using three different functionals (BP86, PBE, and TPSS). The TPSS/DFT‐D3(BJ) yields better geometry, while the BP86 geometry is least accurate for studied complexes. The geometry of platinum complex optimized at TPSS/DFT‐D3(BJ) level is in excellent agreement with the available experimental values. The M–S bonds are shorter than the M–S(O) bonds. The Mayer bond orders suggest the presence of M–S and M–S(O) single bonds. Both the M–S and M–S(O) bond lengths vary with the density functionals as TPSS‐D3(BJ) < TPSS < PBE < BP86. The Hirshfeld charge distribution indicates that the overall charge flows from metal fragment to [S₂O]. The Ni–S₂O bond has greater degree of covalent character than the ionic. The contribution of dispersion interactions is large in computing accurate bond dissociation energies between the interacting fragments. The BDEs are largest for the functional TPSS and smallest for the functional BP86. The DFT‐D3 dispersion corrections to the BDEs between the metal fragments [(PMe₃)₂M] and ligand fragment [(S₂O)] for the TPSS functional are in the range 7.1–7.3 kcal · mol^–1, which are smaller than the corresponding DFT‐D3(BJ) dispersion corrections (9.4–10.6 kcal · mol^–1).     

Hydricity of 3d Transition Metal Complexes from Density Functional Theory: A Benchmarking Study

A range of modern density functional theory (DFT) functionals have been benchmarked against experimentally determined metal hydride bond strengths for three first-row TM hydride complexes. Geometries were found to be produced sufficiently accurately with RI-BP86-D3(PCM)/def2-SVP and further single-point calculations with PBE0-D3(PCM)/def2-TZVP were found to reproduce the experimental hydricity accurately, with a mean absolute deviation of 1.4 kcal/mol for the complexes studied.     

A modern approach for the sensing of aqueous Al(III) ion by Ni(II) Salen‐type Schiff base complexes

In this work, we explore a modern concept of transmetalation (metal exchange) for the effective recognition of aqueous Al(III) ion. Three different Ni(II) salen‐type Schiff base complexes with different spacer diimine groups were prepared for the metal exchange reaction. These probes recognize Al(III) both colorimetically as well as fluorimetrically. The efficiency in sensing is mainly due to the low emission characteristics of the respective Ni(II) complexes which results in enhanced emission on the formation of Al(III) complex. The geometry of the central Ni(II) metal ion in the probe plays a pivotal role in the sensing action with the highest sensitivity being shown by the Ni(II) metal center with distorted square pyramidal geometry. Further DFT calculations and the energetics involved in the sensing mechanism via the formation of Al(III) complexes substantiates the experimental results.     

Structures and energetics of complexation of metal ions with ammonia,water, and benzene: A computational study

Quantum chemical calculations have been performed at CCSD(T)/def2‐TZVP level to investigate the strength and nature of interactions of ammonia (NH₃), water (H₂O), and benzene (C₆H₆) with various metal ions and validated with the available experimental results. For all the considered metal ions, a preference for C₆H₆ is observed for dicationic ions whereas the monocationic ions prefer to bind with NH₃. Density Functional Theory–Symmetry Adapted Perturbation Theory (DFT‐SAPT) analysis has been employed at PBE0AC/def2‐TZVP level on these complexes (closed shell), to understand the various energy terms contributing to binding energy (BE). The DFT‐SAPT result shows that for the metal ion complexes with H₂O electrostatic component is the major contributor to the BE whereas, for C₆H₆ complexes polarization component is dominant, except in the case of alkali metal ion complexes. However, in case of NH₃ complexes, electrostatic component is dominant for s‐block metal ions, whereas, for the d and p‐block metal ion complexes both electrostatic and polarization components are important. The geometry (M⁺–N and M⁺–O distance for NH₃ and H₂O complexes respectively, and cation–π distance for C₆H₆ complexes) for the alkali and alkaline earth metal ion complexes increases down the group. Natural population analysis performed on NH₃, H₂O, and C₆H₆ complexes shows that the charge transfer to metal ions is higher in case of C₆H₆ complexes. © 2016 Wiley Periodicals, Inc.