电子云伸展模型

关于络离子中的价键,本文并不着眼于金属M与配体L之间是否交换电子,而是考虑自由离子波函数进入化学环境后将如何变化。鉴于自由离子与配位场理论中所用的静电排斥参量B、C以及旋-轨偶合参数ζα的定量计算只有在球对称场中才有意义,故有必要建立球对称场的分子轨道理论。     

C_(3v)晶场中d~3离子吸收谱的理论研究

为了计算Cr~(3+)离子在C_(3v)对称晶场中的能谱,本文采用一种形式介于Richardson和Watson SCF波函数之间的束缚态d电子径向轨函;从Oh点群的Griffith标准基出发,用一种简便的方法,推出d~3系的C_(3v)点群强场谱项能量矩阵。由此计算了Ruby(Al_2O_3+Cr~(3+))和Cr_2O_3晶体中Cr~(3+)离子的吸收谱。在考虑扳——电耦合后,理论结果与实验符合甚好,从而解释了这两类晶体中Cr~(2+)吸收光谱的机制。这种计算方法既使拟合参数的数目大为减少,又使配位场理论计算格地理论化。     

块定域波函数方法及其应用

提出了块定域波函数方法以定量分析分子内的电子定域现象或分子间的电荷传递效应。对于一个假想的严格定域的分子,我们通过将全部的电子和基轨道配分成几个子空间来构造其相应的波函数。其中每一个分子轨道只对某一个子空间展开,各子空间内的分子轨道相互正交,但不同子空间内的分子轨道间是非正交的。Hartree-Fock波函数和块定域波函数之间的能量之差即为分子内的电子定域能或分子间的电荷传递能。我们应用块定域波函数方法讨论了丁二烯分子中的旋转势垒。     

高效膦基锇配合物磷光材料的结构和光谱性质

采用B3LYP和UB3LYP方法分别优化了一系列(N^N)2Os(P^P)[P^P=1,2-双(膦基)-甲基,N^N=5-(苯并咪唑-2-基)-3-三氟甲基吡啶(1);ibfpH=5-(1-异丙基-苯并咪唑-2-基)-3-三氟甲基吡啶(2);fppzH=5-(吡啶-2-基)-3-三氟甲基吡啶(3);tfpH=5-(噻唑-2-基)-3-三氟甲基吡啶(4);btfpH=5-(苯基噻唑-2-基)-3-三氟甲基吡啶(5)]配合物的基态和激发态结构.计算得到的Os-P(1),Os-N(1)和Os-N(2)基态键长和相应实验值符合较好.相对于基态,激发态几何结构变化较小,与实验上观察到的斯托克斯频移相一致.配合物1-5的最高占据分子轨道主要由Os的d轨道和N^N配体的π轨道构成,而它们的最低空轨道主要由N^N配体的π反键轨道占据,前线分子轨道能量受N^N配体影响较大.在TD-DFT计算水平下结合PCM溶剂模型,得到配合物1-5的最低能吸收和发射分别在415,416,465,458,481nm和541,538,569,629,655nm.这些跃迁均来自于HOMO→LUMO的激发,具有MLCT/ILCT混合跃迁性质,并且它们的高能吸收也具有相似的跃迁特征.发射波长的巨大差异显示出通过调节N^N配体的π电子捐赠能力可以实现对此类配合物发光颜色的调节.     

卤代硅烷分子的杂化轨道及结构与性质的关系研究

本文利用最大重迭方法,在分别考虑卤素配体的杂化及中央原子Si的d轨道杂化的基础上,计算了卤代硅烷系列分子实验构型下的杂化轨道,研究了卤代硅烷分子的NMR自旋偶合常数,IR伸缩频率和基团电负性与轨道成份的关系,较明确地反映了这类分子的化学键性质对分子谱学性质的影响。     

Ph(SiMe_2)_nPh体系π→π~*UV谱的研究

本文依据Spin-Free理论,使用Gelfand基构造多电子波函数,采用四轨道模型,对Ph(SiMe_2)_nPh体系(n=1～6)的π→π*跃迁进行了EHMO-CI计算,所得第一及第二跃迁能与UV谱的实验结果基本一致。当体系硅链原子数增加时,第一吸收带红移的现象起因于LUMO中d轨道成份增加,导致电子排斥作用变化。在LUMO中,硅链上的d轨道以πd的形式与苯环π~*轨道进行πd—π~*共轭互相作用,这种作用很可能与第一吸收带的强度有内在的联系。     

饱和烃C-H键的活化及其配位催化反应的研究 Ⅲ.PtCl_4~(2-)配位离子催化戊烷氧化氯化反应的EHMO计算

本文用EHMO法计算了饱和烃以端基及侧基配位到催化剂活性种PtCl_3(H_2O)~-的d_(z~2)/d_(x~2-y~2)混合轨道上体系的总能量.结果表明,以端基的方式进行配位较之侧基有利.还计算了反应速率控制步骤中生成过渡态的势垒和主要原子的净电荷的变化,从而阐明了控制步骤的机理是双核配合物分子内靠近氢根配体的桥联氯离子转移到烷基上的还原消去反应.理论计算与实验结果一致.     

铜(Ⅱ)-氨基酸配合物的电子结构研究

用3d轨道径向标度理论解释了一系列铜（Ⅱ）-氨基酸配合物的晶体光谱，并根据配位环境的不同，找出了表征配位情况的参量——非自由度与径向波函数的系数、径向波函数指数因子、旋-轨耦合常数、平均偶极矩和d－d谱的重心位置的关系，对其光谱序列作了理论解释。为今后预测配合物的配住环境提供了一种简便方法，即根据配合物电子吸收光谱的重心位置来预知其大致结构。     

金属四重键化合物M2X4(PMe3)4(M=Cr,Mo,W;X=F,Cl,Br,I)结构和电子光谱的密度泛函理论研究

采用密度泛函理论方法,在TZ2P-STO基组水平下,对金属四重键化合物M2Cl4(PMe3)4(M=Cr,Mo,W)和Mo2X4(PMe3)4(X=F,Cl,Br,I)的几何结构进行优化,分析了电子结构,并运用TDDFT方法对其低占据激发态进行了计算.考虑相对论效应的ZORA方法能够较好地重现M2X4(PMe3)4的几何结构.M2X4(PMe3)4的电子结构分析表明其d电子的组态为σ2π4δ2,前线轨道能级顺序为πlig<πd/σd<δd<δd*.金属原子和卤素配体的改变虽然使轨道能量发生变化,但没有影响轨道的排布顺序.TDDFT方法对M2X4(PMe3)4δd→δd*和πd→δd*跃迁能量的计算较为准确,对πlig→δd*(LMCT)跃迁能量的计算误差较大.金属原子、卤素配体以及相对论效应对激发能的影响可以根据分子轨道能级的变化给予解释.     

非血红素配合物[FeⅣ(O)(TMC)(NCMe)]2+与[FeⅣ(O)(TMCS)]+的几何结构、电子结构、成键性和反应活性比较

采用密度泛函理论计算了[FeⅣ(O)(TMC)(NCMe)]2+ 和[FeⅣ(O)(TMCS)]+的电子结构、反应活性和Fe—O的成键性. 几何构型的优化采用非限制性的B3LYP混合密度泛函方法, 重原子Fe的优化采用是LanL2dZ基组, C, H, O, N和S的优化采用TZV基组, 理论计算结果与实验结果相符. 通过对轨道系数和键级的分析发现, TMC配位基对Fe—O的π键几乎没有影响. 由于竖直方向的硫甲基配位基的轨道与Fe的3d轨道具有较强的重迭, 而乙腈配位基作为轴向配体时, 这种重迭则小得多, 导致了两种配合物在电子结构和反应活性上存在一定的差别.     

稀土乙酰丙酮络合物的激光拉曼和红外光谱(Ⅰ)

本文测定了15个一水稀土乙酰丙酮络合物的激光拉曼和红外光谱,在401、415cm~(-1)附近的拉曼谱带对不同稀土离子表现敏感,它们随原子序数变化呈现“四分组”效应,这是第一次在振动光谱中观察到的镧系递变规律。该系列络合物的振动频率变化亦符合镧系“斜W”效应的规律,这些特征规律为确认401、415cm^-1附近谱带为M-O拉伸振动提供了最好的证据。实验结果同时可用于讨论M-O键的性质。     

Density functional study of guanine and uracil quartets and of guanine quartet/metal ion complexes

The structures and interaction energies of guanine and uracil quartets have been determined by B3LYP hybrid density‐functional calculations. The total interaction energy ΔE^T of the C_4h‐symmetric guanine quartet consisting of Hoogsteen‐type base pairs with two hydrogen bonds between two neighbor bases is −66.07 kcal/mol at the highest level. The uracil quartet with C6 H6O4 interactions between the individual bases has only a small interaction energy of −20.92 kcal mol⁻¹, and the interaction energy of −24.63 kcal/mol for the alternative structure with N3 H3O4 hydrogen bonds is only slightly more negative. Cooperative effects contribute between 10 and 25% to all interaction energies. Complexes of metal ions with G‐quartets can be classified into different structure types. The one with Ca²⁺ in the central cavity adopts a C_4h‐symmetric structure with coplanar bases, whereas the energies of the planar and nonplanar Na⁺ complexes are almost identical. The small ions Li⁺, Be²⁺, Cu⁺, and Zn²⁺ prefer a nonplanar S₄‐symmetric structure. The lack of coplanarity prevents probably a stacking of these base quartets. The central cavity is too small for K⁺ ions and, therefore, this ion favors in contrast to all other investigated ions a C₄‐symmetric complex, which is 4.73 kcal/mol more stable than the C_4h‐symmetric one. The distance 1.665 Å between K⁺ and the root‐mean‐square plane of the guanine bases is approximately half of the distance between two stacked G‐quartets. The total interaction energy of alkaline earth ion complexes exceeds those with alkali ions. Within both groups of ions the interaction energy decreases with an increasing row position in the periodic table. The B3LYP and BLYP methods lead to similar structures and energies. Both methods are suitable for hydrogen‐bonded biological systems. Compared with the before‐mentioned methods, the HCTH functional leads to longer hydrogen bonds and different relative energies for two U‐quartets. Finally, we calculated also structures and relative energies with the MMFF94 forcefield. Contrary to all DFT methods, MMFF94 predicts bifurcated C HO contacts in the uracil quartet. In the G‐quartet, the MMFF94 hydrogen bond distances N2 H22N7 are shorter than the DFT distances, whereas the N1 H1O6 distances are longer. © 2000 John Wiley & Sons, Inc. J Comput Chem 22: 109–124, 2001     

Enrichment of copper and nickel with solid phase extraction using multiwalled carbon nanotubes modified with Schiff bases

The behaviour of some Schiff bases in the presence of metal ions is very selective in complex formation. In this study, new, selective and easily prepared adsorbent materials have been developed. Multiwalled carbon nanotubes (MWCNTs) are quite suitable as supporting material for preparation of new solid phase adsorbents modified with Schiff bases due to their selective nature. Different Schiff bases were designed and synthesised as adsorbent agents for Ni(II) and Cu(II) ions, according to the literature, and MWCNTs were modified with these Schiff bases. The modification of CNTs was performed by adsorption from the alcoholic solution of Schiff base. The measurements of Ni(II) and Cu(II) ions were carried out using ICP-MS. Different parameters such as pH, model and eluent solution flow rates, eluent type, amount of ligand, sample volume and effect of foreign ions, which have an effect upon recovery of analytes, were investigated. The obtained results indicated that enrichment can be done with six modified adsorbent materials for Cu(II) at pH 9 and two modified adsorbent materials for Ni(II) at pH 8. It was concluded that four adsorbent materials were selective only for the enrichment of Cu(II). Merely one modified adsorbent material was noneligible for the enrichment of Cu(II) and Ni(II). The solid phase adsorbents prepared by modification with two of the Schiff bases used in this study showed an enrichment factor of 80 for both metal ions, whereas the solid phase adsorbents prepared by modification with four of the Schiff bases showed an enrichment factor of 40 for Cu(II) ions. The confirmation of the developed method was tested with certified reference materials with satisfactory results.     

Intermediate-spin state of a 3d ion in the octahedral environment and generalization of the Tanabe-Sugano diagrams

Electronic spectra of 3d(n) transition ions in an octahedral ligand surrounding have been studied using the modified crystal field approach (MCFA), which includes a relativistic spin-orbital interaction. A new variable parameter, the effective nuclear charge Z(eff) of a metal ion that allows accounting implicitly the covalence degree of a metal-ligand bond, has been introduced. Energy diagrams similar to the Tanabe-Sugano ones have been calculated. To study the spin state evolution of the metal ion in an arbitrary distorted octahedral complex, a spin state diagram approach has been proposed. The intermediate-spin (IS) state problem for 3d(4), 3d(5), and 3d(6) metal ions has been considered and conditions for the IS state realization have been formulated. The regions of the mixed high-, intermediate-, and low-spin states have been found. The possibility of coexistence of the different spin states of 3d ions in the octahedral complexes has been considered using crystallography data for the YBaCo(2)O(5.5) layered cobaltite.     

Dynamical symmetry analysis of ionization and harmonic generation of atoms in bichromatic laser pulses

Recently the effect of the relative phase ? in a high‐intensity (～10¹⁴ W/cm²) two‐color (bichromatic) CW laser with frequencies ω and 2ω on the high‐order harmonic generation (HHG) was studied within the framework of the non‐Hermitian quantum mechanics (NHQM) [Phys Rev A 2004, 69, 043404/1]. Here we emphasize the study of symmetries in bichromatic HHG spectra within the framework of the conventional Hermitian QM, and in particular by taking the duration of the laser pulse into consideration (an effect that has not been included in the non‐Hermitian studies due to the time asymmetry problem in NHQM). The phase dependence of HHG and intense‐field ionization probability in a 1D Xe atom with symmetric field‐free potential and symmetric initial wave function were studied numerically and analytically. From simulations based on a single‐particle response it can be seen that the HHG spectra is symmetric with respect to inversion in the relative phase between the two colors ? only if ionization is forbidden in the system and the laser pulse is an adiabatic one. The HHG spectra is symmetric with respect to a π‐shift in ? whenever the laser pulse is an adiabatic one, either for bound or open (ionized) systems. The ionization probability is symmetric both to inversion or π‐shift in ?; the component probabilities (right‐ and left‐ionization probabilities) have the same ?‐dependence, up to a shift of π. © 2005 Wiley Periodicals, Inc. Int J Quantum Chem, 2005     

An application of perturbation theory ideas in configuration interaction calculations

Configuration interaction calculations of electronic wave functions for atoms and molecules have generally been limited to relatively small basis sets because of the exponential increase in the number of configurations as basis functions are added. While higher than quadruply excited configurations are of negligible importance in CI wave functions, it is shown that the effect of triple and quadruple excitation configurations can be substantially included even when the matrix elements between such configurations are neglected, leaving only their diagonal elements and the elements connecting them with the single and double excitations. This approximation is seen to be formally practically equivalent to a first-order perturbation expression for the wave function (second-order for the energy) based on an optimum linear combination of the zero, single, and double excitation configurations as the zero-order function. If suitable procedures are used, the amount of computational effort involved in such a calculation is roughly proportional to the fourth power of the number of basis functions employed, thus preventing the CI stage of the calculation from increasing in magnitude much faster than the stages involving the calculation and manipulation of the elementary integrals.     

过渡金属离子的掺杂对TiO2光催化活性的影响

考察了过渡金属离子对TiO₂ 光催化性能的影响,结果发现:第二过渡系列金属离子对TiO₂ 膜的修饰作用比第一过渡系列金属离子的修饰作用更加明显;第二、六副族的金属离子对TiO₂ 膜的修饰效果较好.通过X射线衍射(XRD)、电镜分析 (SEM)、光电能谱分析 (XPS)及差热分析 (DTA)对催化剂表面进行了表征,结果表明:TiO₂ 的晶型为锐钛矿型,粒子半径为 32.58nm.     

Influence of Mg2+ and Cd2+ on the interaction between sparfloxacin and calf thymus DNA

Mg(2+) and Cd(2+) have different binding capacity to sparfloxacin, and have different combination modes with calf thymus DNA. Selecting these two different metal ions, the influence of them on the binding constants between SPFX and calf thymus DNA, as well as the related mechanism have been studied by using absorption and fluorescence spectroscopy. The result shows that Cd(2+) has weak binding capacity to SPFX in the SPFX-Cd(2+) binary system, but can decrease the binding between SPFX and DNA obviously in SPFX-DNA-Cd(2+) ternary system. Mg(2+) has strong binding capacity to SPFX. It can increase the binding between SPFX and DNA at concentrations <0.01 mM, and decrease the binding between them at concentrations >0.01 mM. Referring to the different modes of Mg(2+) and Cd(2+) binding to DNA, the mechanism of the influence of metal ions on the binding between SPFX and DNA has been proposed. SPFX can directly bind to DNA by chelating DNA base sites. If a metal ion at certain concentration mainly binds to DNA bases, it can decrease the binding constants between SPFX and DNA through competing with SPFX. While if a metal ion at certain concentration mainly binds to phosphate groups of DNA, it can increase the binding constants by building a bridge between SPFX and DNA. The influence direction of metal ions on the binding between quinolone and DNA relays on their binding ratio of affinity for bases to phosphate groups on DNA. Our result supports Palumbo's conclusion that the binding between SPFX and the phosphate groups is the precondition for the combination between SPFX and DNA, which is stabilized through stacking interactions between the condensed rings of SPFX and DNA bases.     

新型荧光试剂N-2-噻唑基水杨醛亚胺Schiff碱的合成及荧光性质

合成了１０种新型荧光试剂Ｎ－２－噻唑基水杨醛亚胺Ｓｃｈｉｆ碱,通过元素分析,ＩＲ,１ＨＮＭＲ和ＵＶ－ｖｉｓ光谱进行了结构表征,并且测定了试剂的荧光光谱,微量的二价碱土金属离子对试剂的荧光有一定的熄灭作用