单核Cu(Ⅱ)配合物C_(18)H_(12)CuN_4O-2的密度泛函研究

用量子化学从头算方法,在ROB3LYP/LANL2MB水平上,对单核配合物C18H12CuN4O2进行了理论计算,优化得到了该配合物的平衡几何构型,并计算了它的谐振动频率.结果表明:该配合物分子是可以稳定存在的,电子自旋布居主要集中在Cu原子及配体原子上,Cu原子和配体原子的自旋布居符号相同,说明体系中存在较强的自旋离域效应.体系的前沿轨道主要由Cu原子的d轨道和配体原子的p轨道组成,这种组成有利于配体与磁中心之间的电子转移.计算结果与实验符合得较好.     

二硫代草酰胺基或二环己酮草酰二腙作桥联基的新型双核Cu（Ⅱ）－Cu（Ⅱ）配合物的合成和磁性（Ⅱ）

合成和表征了四种新的以二硫代草酰胺基（ｄｔＯ２－）或二环己酮草酰二腙（ＢＣＯ）作桥基的双核金属配合物［Ｃｕ２（ｐｈｅｎ）２（ｄｔＯ）］（ＣｌＯ４）２（１）、［Ｃｕ２（ｄｉｅｎ）２（ｄｔＯ）］（ＣｌＯ４）２·２Ｈ２Ｏ（２）、［Ｎｉ２（ｄｉｅｎ）２（Ｈ２Ｏ）２（ｄｔＯ）］（ＣｌＯ４）２（３）及［Ｃｕ２（ｐｈｅｎ）２（ＣｌＯ４）２（ＢＣＯ）］（ＣｌＯ４）２（４），（ｐｈｅｎ：１，１０－邻菲咯啉，ｄｉｅｎ：二乙烯三胺）。测定了配合物１和４的变温磁化率，并求出交换积分Ｊ分别为－７．６７（１）和－０．９２（４）ｃｍ－１，表明双核配合物中铜离子间存在反铁磁性自旋交换相互作用。     

牛磺酸缩邻香草醛席夫碱铜配合物[Cu（C12H8N2）（C10H11NO5S）]·3．5H2O的合成及晶体结构

含硫席夫碱及其金属配合物具有抑菌、抗癌和抗病毒的生物活性,有些含O、N席夫碱金属配合物具有仿酶催化活性。而氨基酸席夫碱配合物具有良好的生理活性,近年来得到人们的普遍重视。2-氨基乙磺酸（牛磺酸）作为生物体内一种特殊的氨基酸,对它的研究主要集中在生理和病理方面,     

新颖双核铜配合物[Cu2（C7H（19）N3O）2（C（10）H8N2）]（ClO4）4·H2O的合成、晶体结构及表征

生物体内由金属离子构成的水解酶的活性中心结构和催化机理是生物无机化学领域研究的热点问题。在天然水解酶中,锌离子被认为是结合底物和亲核基的催化活性中心,它可以活化底物的羰基或水分子。而在模拟酶研究中发现,含其它金属离子活性中心的某些有机配合物具有相似于水解酶的催化活性。解永树等研究了含醇羟基和酚羟基链型氮氧杂配体与Cu（Ⅱ）的配合物催化NA酯的水解动力学。1．[二（2-氨基乙基）氨基1．2-丙醇是带羟基臂的重要的有机多胺配体,     

[Mo（H2O）4{NCS）2].（18—C—6）配合物晶体的电子结构与成键特性理论研究

本文取配合物晶体[Mn(H2O)4(NCS)2].(18-C-6)的一个分子片断进行CNDO／2半经验分子轨道理论计算，给出Mulliken键级，电荷分布和电子态密度等，探讨了其成键特性，结果表明，过渡金属配合单元[Mn(H2O)4(NCS)2]与18－C－6冠醚环之间的主要结合方式是定域化程度相当高的氢键，与来自实验测量的推测相一致。     

配合物VO[(C15H12N2O4)(OC2H5)]的合成晶体结构和氧化还原性质

含有ONO给体原子的N-邻甲氧基苯甲酰基水杨酰肼配体与[VO(acac)2]在乙醇中反应得到钒(V)酰配合物VO[(C15H12N2O4)(OC2H5)].标题化合物晶体属三斜晶系,空间群Pī,晶胞参数:a＝0.894 11(5)nm,b＝1.006 3(2)nm,c＝1.039 2(2)nm,α＝110.171(7)°,β＝95.219(3)°,γ＝93.822(2)°;V＝0.869 2(2)nm3,Z＝2,R1＝0.051 3,wR＝0.153 2.研究结果表明:钒原子具有扭曲的四方锥配位构型,钒酰氧原子处在锥顶位置,配体的3个给体原子与溶剂分子形成锥底平面.     

IB 族金属-乙烯配合物[N{(Me)C(Ph)N}2]M-C2H4 (M=Cu,Ag, Au)的电子结构

采用从头算Hartree-Fock(HF),M??ller-Plesset微扰(MP2),二级近似耦合簇(CC2)和密度泛函理论(DFT)方法,对IB族金属-乙烯配合物LM-C2H4(L=[N{(Me)C(Ph)N}2];M=Cu,Ag,Au)的几何结构、电子结构以及LM与C2H4之间的结合能进行了理论研究.MP2、CC2和密度泛函方法对C2H4配位前后C=C键长的变化情况都给出了正确的描述.电子结构分析显示LM与C2H4之间主要以C2H4→LM"σ-给予"和LM→C2H4"π-反馈"方式协同成键,这种成键方式使C2H4配体π轨道上的电子密度下降,π*轨道上的电子密度增加,并使得C=C键长增加、键能下降,从而达到活化C=C键的目的.自然电荷布居和能量分解分析显示LM-C2H4中的"σ-给予"作用弱于"π-反馈"作用,若使用"σ-给予"作用强于"π-反馈"作用的M+-C2H4体系作为LM-C2H4的简化模型进行理论研究是不合适的.LM-C2H4中金属原子M的改变对C=C键长、C2H4电荷布居以及LM与C2H4之间的结合能等性质影响显著.LAu与LCu、LAg相比其接受和反馈电子的能力最强,使C2H4配体π轨道电子密度减少的程度和π*轨道电子密度增加的程度也最大,因此LAu对C2H4中C=C键的活化效果最好.螯合配体取代基供、吸电能力的改变对上述性质的影响则非常有限.     

双核Cu（Ⅱ）、Ni（Ⅱ）与N—氧化—2，6—二甲酰吡啶Schiff碱大环配合物的合成和表征

Robson和Okaw等用2,6-二甲酰-4-取代的酚和合适的多胺缩合成了一系列的大环双核配体及其双核配合物(a),并对双核过渡金属配合物的光谱和磁性进行了研究。但迄今为止,国内外尚未见到有关N-氧化-2,6-二甲酰吡啶和多胺缩合生成大环配体及其配合物的报道。为研究大环双核体系中不同桥连原子对金属间磁相互作用的影响,我们首次以N-氧化-     

低阶煤半焦利用热重在O2/CO2、O2/N2和O2/Ar气氛下燃烧特性研究

利用热重研究了两种中国西北典型低阶煤半焦的燃烧特性。探究了不同气氛（O₂/CO₂、O₂/N₂和O₂/Ar）和不同氧气浓度对其燃烧特性的影响。实验结果表明,无论是反应气氛还是氧气浓度都会对低阶煤半焦的燃烧产生影响。相比于N₂和Ar,CO₂明显有利于燃烧反应进行：当反应气氛由O₂/CO₂变为O₂/Ar时,两种不同低阶煤半焦的燃尽温度分别升高了63.7和68.8℃;而当反应气氛由O₂/CO₂变为O₂/N₂时,两种不同低阶煤半焦的燃尽温度分别升高了135.9和129.6℃。在研究范围内,氧气浓度的提高也能明显提高半焦的燃烧性能。与此同时,半焦燃烧特性的动力学分析表明,随着氧气浓度提高,两种半焦燃烧反应的表观活化能E和指前因子A均呈增大趋势。通过对E和A两者关系的分析结果表明,半焦富氧燃烧的活化能和指前因子存在动力学补偿效应。     

Oxygen analysis of O2MF6 and O2M2F11 salts

The dioxygenyl salts O₂MF₆ or O₂M₂F₁₁ where M = As, Sb, Bi, Nb, Ta, Ru, Au, and Pt, were hydrolysed aqueous base (40% NaOH) to evaluate their purity and to gain further information about their thermal instability. Compounds containing As, Sb, Bi, Nb and Ta yielded 1.25 moles O₂ per mole of starting material whereas for compounds containing Ru, Au and Pt, 1.5 moles of O₂ per mole of salt was produced. The difference is a consequence of the greater oxidizing power of the RuF^-₆, AuF^-₆ and PtF^-₆ anions. All of the dioxygenyl salts are intrinsically unstable at room temperature in vacuum.     

Li1.2Mn0.54Ni0.13Co0.13O2正极材料的Ga2O3包覆改性及电化学性能

首先采用共沉淀方法制备富锂锰基正极材料 Li_1.2Mn_0.54Ni_0.13Co_0.13O₂原始样品(P-LRMO), 然后通过简单的湿化学法以及低温煅烧方法对其进行不同含量 Ga₂O₃原位包覆。透射电子显微镜(TEM)以及 X射线光电子能谱(XPS)结果表明在 P-LRMO表面成功合成了 Ga₂O₃包覆层。电化学测试结果表明:含有 3 %Ga₂O₃的改性材料 G3-LRMO具有最优的电化学性能, 其在 0.1C倍率(电流密度为 25 mA·g^-1)下首圈充放电比容量可以达到 270.1 mAh·g^-1, 在 5C倍率下容量仍能保持 127.4 mAh·g^-1, 优于未改性材料的 90.7 mAh·g^-1, 表现出优异的倍率性能。G3-LRMO在 1C倍率下循环 200圈后仍有 190.7 mAh·g^-1的容量, 容量保持率由未改性前的 72.9 %提升至 85.6 %, 证明 Ga₂O₃包覆改性能有效提升富锂锰基材料的循环稳定性。并且, G3-LRMO在 1C倍率下循环 100圈后, 电荷转移阻抗(R_ct)为 107.7 Ω, 远低于未改性材料的 251.5 Ω, 表明 Ga₂O₃包覆层能提高材料的电子传输速率。     

CH2+O2反应的反应机理

The mechanisms of the CH2＋ O2→ H2O＋ CO and CH2＋ O2→ H2＋ CO2 reactions have been studied by performing ab initio CAS(8,8)/6-31G(d,p) calculations, and five intermediates(IMn) and eight transitions(TSn) have been located along the reaction paths. The predicted path for the CH2＋ O2→ H2O＋ CO is: CH2＋ O2→ TS1→ IM1→ TS2→ IM2→ TS3→ IM3→ TS4→ IM4a→ TS5→ H2O＋ CO. For the CH2＋ O2→ H2＋ CO2 reaction, there are two paths: (i) CH2＋ O2→ TS1→ IM1→ TS2→ IM2→ TS3→ IM3→ TS6→ H2＋ CO2 and (ii) CH2＋ O2→ TS1→ IM1→ TS2→ IM2→ TS3→ IM3→ TS4→ IM4a→ TS7→ IM4b→ TS8→ H2＋ CO2, with the latter path more favorable energetically.     

Rate coefficients for CS reactions with O2, O3 and NO2 AT 298 K

CS radicals have been produced by photodissociation of CS₂ at 193 nm and their disappearance monitored by LIF. The vibrationally excited CS radicals rapidly relax to CS(ν = 0). At 298 K, the rate coefficients for CS(ν = 0) reactions with O₂, O₃ and NO₂ are (2.9 ± 0.4) × 10_?19, (3.0 ± 0.4) × 10^?16 and (7.6 ± 1.1) × 10^?17 cm³ molecule^?1 s^?1 respectively. The quenching of CS(A ¹II)_ν=0 by He has a rate coefficient of (1.3 ± 0.2) × 10^?12 cm³ molecule^?1 s^?1.     

Intermolecular forces for D2, N2, O2, F2 and CO2

The intermolecular potentials for D₂, N₂, O₂, F₂ and CO₂ are determined on the basis of the second virial coeffincients, the polarizabilities parallel and perpendicular to the molecular axes, and the electric quadrupole moment. The repulsive parts of the potentials are taken from the corresponding Kihara core-potentials. Effects of the octopolar induction are taken into consideration in a unique way. The potential depends on relative orientations of the two molecules as well as the distance r between the molecular centers. This dependence is shown in graphs. A measure of the anisotropy of the potential depth is 0.72 for CO₂ 0.36 for D₂, and smaller than 0.27 for N₂ O₂ and F₂. The remarkable anisotropy for CO₂ and D₂ is due to strong electrostatic quadrupole interactions.     

Vibrational spectra of the peroxotantalates (NH4)3[Ta(O2)4], K3[Ta(O2)4], Rb3[Ta(O2)4] and Cs3[Ta(O2)4] and the crystal structure of Rb3[Ta(O2)4]

The compounds (NH₄)₃[Ta(O₂)₄], K₃[Ta(O₂)₄], Rb₃[Ta(O₂)₄] and Cs₃[Ta(O₂)₄] have been prepared and investigated by X-ray powder methods as well as Raman- and IR-spectroscopy. In the case of Rb₃[Ta(O₂)₄] the structure has been solved from single crystal data. It is shown that all these compounds are isotypic and crystallize in the K₃[Cr(O₂)₄] type (SG , No. 121). The infrared- and Raman spectra (recorded on powdered samples) are discussed with respect to the internal vibrations of the peroxo-group and the dodecahedral [Ta(O₂)₄]³⁻ ion. Symmetry coordinates for the [Ta(O₂)₄]³⁻ ion are given from which the vibrational modes of the O-O stretching vibrations of the O₂²⁻ groups, the Ta-O stretching vibrations and the Ta-O bending vibrations are deduced.     

Solid state photodecomposition studies of K4Ti(O2)4·2H2O, K3Ta(O2)2F4 and K2V2O3(O2)2F2

The compounds K₄Ti(O₂)₄·2H₂O, K₃Ta(O₂)₂F₄ and K₂V₂O₃(O₂)₂F₂ undergo photolysis in the solid state. The photolysis kinetics obey the parabolic rate equation p = kt^1/2 and indicate a monoexcitation process for the photolysis. These features are similar to those reported previously for peroxo complexes. The mechanism of evolution of oxygen reported earlier appears to be the same in all these solids.     

Effect of CO2 on O2 photo-adsorption on anatase

The presence of CO₂ on TiO₂ affects the process of oxygen photo-adsorption depending on the hydroxylation state of the surface. In dehydroxylated samples CO₂ blocks the formation of O ₃ ^– and O ₂ ^– . On H₂O₂/TiO₂ samples pretreated in the range of 150–200°C it leads to CO₂–O ₂ ^– species.

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