吡啶-2-甲醛肟钛氧簇合物的合成、结构调控及光电性质

通过溶剂热合成方法,以吡啶-2-甲醛肟（HPycox）和Ti（OⁱPr）₄合成了双核钛配合物[Ti₂（μ₂-O）（Pycox）₂（OⁱPr）₄] （1）。通过结构分析,分别使用二苯基膦酸和苯基膦酸对其进行结构调控,成功制备了三核钛配合物[Ti₃（μ₂-O）₂（Pycox）₂（Ph₂PO₂）₂（OⁱPr）₄] （2）和六核钛配合物[Ti₆（μ₂-O）₂（μ₃-O）₂（Pycox）₂（PhPO₃）₄（OⁱPr）₆]·2CH₃CN （3）。配合物1~3的光学带隙分别为2.89、3.00和2.87 eV,其中配合物2的光电流密度可达0.1 μA·cm^-2。     

香草醛缩多胺Schiff碱Co(II)配合物固相合成及氧合性能研究

采用固相反应合成了三个新的席夫碱钴(II)配合物, 在室温下, 将其与O₂作用, 1 mol配合物吸收2 mol O₂, 得到三种固态氧合配合物[Co•(L₁)₂•(O₂)₂](NO₃)₂•2H₂O [L₁＝N,N-二(4-羟基-3-甲氧基苯亚甲基)二乙烯三胺], [Co•(L₂)₂•(O₂)₂](NO₃)₂•2H₂O [L₂＝N,N-二(4-羟基-3-甲氧基苯亚甲基)三乙烯四胺]和[Co•(L₃)₂•(O₂)₂](NO₃)₂•2H₂O (L₃＝N,N-二(4-羟基-3-甲氧基苯亚甲基)四乙烯五胺]. 通过元素分析、红外光谱、核磁共振氢谱(¹H NMR), TG/DTA、摩尔电导率、紫外等测试手段确定了氧合配合物的组成. 采用失重法测定了氧合配合物中的配位氧, 确定1 mol钴配合物吸收2 mol O₂, 其中1 mol O₂用来和钴离子配位形成超氧配合物.     

香草醛缩多胺Schiff碱Co(II)配合物固相合成及氧合性能研究

采用固相反应合成了三个新的席夫碱钴(II)配合物, 在室温下, 将其与O₂作用, 1 mol配合物吸收2 mol O₂, 得到三种固态氧合配合物[Co•(L₁)₂•(O₂)₂](NO₃)₂•2H₂O [L₁＝N,N-二(4-羟基-3-甲氧基苯亚甲基)二乙烯三胺], [Co•(L₂)₂•(O₂)₂](NO₃)₂•2H₂O [L₂＝N,N-二(4-羟基-3-甲氧基苯亚甲基)三乙烯四胺]和[Co•(L₃)₂•(O₂)₂](NO₃)₂•2H₂O (L₃＝N,N-二(4-羟基-3-甲氧基苯亚甲基)四乙烯五胺]. 通过元素分析、红外光谱、核磁共振氢谱(¹H NMR), TG/DTA、摩尔电导率、紫外等测试手段确定了氧合配合物的组成. 采用失重法测定了氧合配合物中的配位氧, 确定1 mol钴配合物吸收2 mol O₂, 其中1 mol O₂用来和钴离子配位形成超氧配合物.     

苯甲醛缩三乙烯四胺Schiff碱Co(Ⅱ)配合物固相合成及氧合性能研究

Three new cobalt complexes were synthesized by solid-state reaction at room temperature. It was found that one mole of complex reacted with two moles of oxygen at room temperature. And the oxygenated complexes [Co·(L₁)₂·2O₂](NO₃)₂·2H₂O (L₁=N,N′-bis(4-hydroxyl-3-methoxy-benzyl)-triethylenetetramine), [Co·(L₂)₂·2O₂](NO₃)₂ ·2H₂O (L₂=N,N′-bis(4-hydroxyl-benzyl)-triethylenetetramine) and [Co·L₃·2O₂](NO₃)₂·2H₂O (L₃=N,N′-bis(2-hydroxyl-benzyl)-triethylenetetramine) were obtained and characterized by elemental analysis, IR spectra, ¹H NMR, TG/DTA, UV-Vis and molar conductance. The coordinated oxygen contents in the oxygenated complex were also determined by weight method. It was found that one O₂ molecule coordinated to the Co ion and formed superoxo type oxygenated complex.     

酚氧桥联多核铜(Ⅱ)配合物的合成、结构和磁性

利用柔性酚胺类配体N,N'-二甲基-N,N'-(2-羟基-4,5-二甲基苄基)乙二胺(H₂L)与Cu(Ⅱ)反应,合成了2个新的酚氧桥联多核Cu(Ⅱ)配合物[Cu₃^II(L)₂(CH₃OH)₂](ClO₄)₂(1),[Cu₃^II(L)₂(Cu^ICl₂)₂](2)。配合物1~2中,3个Cu²⁺之间通过2个酚氧桥连接,形成线性三核结构。两边的铜离子分别被配体L^2-上的N₂O₂螯合配位,轴向与甲醇分子的氧(配合物1)或[CuCl₂]^-的氯(配合物2)配位,形成四方锥配位构型。中间铜离子与两侧L^2-上的4个酚氧原子以平面四边形配位。Cu^II-O-Cu^II键角为100.14°~101.79°。对配合物1~2进行变温磁化率测量表明,铜离子之间通过酚氧桥存在强的反铁磁耦合,磁耦合常数J分别为-277(9)cm^-1(配合物1)和-299(3)cm^-1(配合物2)(基于自旋哈密顿算符Ĥ=-2J(Ŝ₁·Ŝ₂+Ŝ₂·Ŝ₃)。J值与酚氧桥桥联键角有一定相关性,即Cu-O-Cu桥联键角越大,反铁磁耦合越强。     

含乙酰氧肟酸配体的席夫碱钒配合物的合成、结构及其抑制幽门螺旋杆菌脲酶研究

本文合成了2个新的含乙酰氧肟酸配体的席夫碱钒配合物,[V^ⅢL¹(HAHA)](1)和[V^ⅤOL²(AHA)](2),其中L¹为N,N’-二(5-甲基水杨基)乙烷-1,2-二胺的二价阴离子,L²为2-{[2-(2-羟乙基氨基)乙亚胺基]甲基}-6-甲基苯酚的一价阴离子,HAHA和AHA分别为乙酰氧肟酸的一价和二价阴离子,通过物理-化学方法以及单晶X-射线衍射表征了它们的结构。在每个化合物中,V原子都采取八面体配位构型。本文还研究了配合物的热稳定性以及其对幽门螺旋杆菌脲酶的抑制活性。在浓度为100μmol·L^-1时,配合物1和2对脲酶的抑制率分别为37.2%和81.5%,其中配合物2的IC₅₀值为21.5μmol·L^-1。分子对接研究表明配合物2与脲酶活性中心存在有效的作用力。     

两个具有Sn4O8簇结构的二丁基锡芳氧乙酸酯配合物的合成、晶体结构及除草活性

以二丁基氧化锡分别与苯氧乙酸(L1)、邻氯苯氧乙酸(L2)反应，合成了2个四核二丁基锡芳氧乙酸酯配合物[(o-R—C₆H₄—OCH₂COOSn(n-Bu)₂)₂O]₂(R=H (C1)、Cl (C2))。经元素分析、IR、¹H和¹³C NMR以及X射线单晶衍射表征其结构。在配合物C1、C2的独立分子中，分别存在1个以Sn₂O₂平面四元环为中心的Sn₄O₄梯形结构，梯的两侧分别由羧基的2个O原子与梯边的Sn—O—Sn链桥联成六元环，形成一个含Sn₄O₈的锡氧簇结构。配合物在220℃(C1)、250℃(C2)的空气气氛下具有较好的热稳定性。除草活性结果表明，配合物C1对决明具有较好的生长调节作用，配合物C2在50 mg·L^-1浓度下可高效、选择性地抑制刺苋的茎和根的生长。     

基于2-吡啶甲醛肟配体的NiⅡ2ZnⅡ2簇配合物的合成、晶体结构、磁性及光催化性能

在溶剂热条件下，以2-吡啶甲醛肟(HL)为主配体，Zn(OAc)₂·2H₂O和NiCl₂·6H₂O为金属盐，合成了一个Ni^Ⅱ₂Zn^Ⅱ₂簇配合物[Ni₂Zn₂(L)₄Cl₂(CH₃O)₂](1)，通过元素分析、红外光谱、单晶X射线衍射等对其结构进行了表征。研究了该配合物的磁性及光催化降解染料的性能，结果表明：配合物1属于正交晶系，Pna2₁空间群，其分子中包含2个Ni^Ⅱ离子，2个Zn^Ⅱ离子，4个L-配体，2个Cl^-离子和2个CH₃O^-离子。磁性研究表明Ni^Ⅱ…Ni^Ⅱ离子间存在弱的反铁磁相互作用。光催化降解染料的研究结果表明该配合物对甲基橙和罗丹明B有较好的降解活性，降解率分别达到83.9%和71.1%。进一步探讨了光催化降解染料的作用机理。     

双烷氧桥联的双核铜(Ⅱ)Schiff碱配合物的合成及配合行为

通过Salen型双肟配体H₂L¹(H₂L¹=5,5′-二(N,N′-二乙胺)-2,2′-[乙二氧双(氮次甲基)]二酚)与乙酸铜反应,合成了一种双核铜(Ⅱ)配合物[Cu₂(L²)₂](H₂L²=4-(N,N′-二乙胺)水杨醛O-(2-羟乙基)肟),并对其进行了X-射线衍射单晶结构分析。     

3,6-二(N-咪唑/苯并咪唑基)哒嗪配体配合物的合成、结构、荧光及光催化性能

用溶剂热法设计、合成了4个金属-有机配合物[Mn(L¹)₄(OH)₂](1),{[MnL¹(H₂O)₄]SO₄}_n(2),[CdL²(NO₃)₂]_n(3)和{[Co(L²)₂](PF₆)₂}_n(4),(L¹=3,6-二(N-咪唑基)哒嗪,L²=3,6-二(N-苯并咪唑基)哒嗪),并通过元素分析、红外、X射线单晶衍射对配合物结构进行了表征,测试结果表明配合物1具有单核结构,2为一维链结构,配合物3和4均为二维网状结构。此外,对配合物3和4的固态荧光性能及光催化的性能做了进一步研究。     

Solid-solid interactions in pure and Li2O-doped manganese and magnesium mixed oxides system

The solid-solid interactions between manganese and magnesium oxides in absence and in presence of small amounts of Li₂O have been investigated. The molar ratios between manganese and magnesium oxides in the form of Mn₂O₃ and MgO were varied between 0.05:1 to 0.5:1. The mixed solids were calcined in air at 400-1000°C. The techniques employed were DTA, XRD and H₂O₂ decomposition at 20-40°C.The results obtained revealed that solid-solid interactions took place between the reacting solids at 600-1000°C yielding magnesium manganates (Mg₂MnO₄, Mg₆MnO₈, MgMnO₄ besides unreacted portions of MgO, Mn₂O₃ and Mn₃O₄). Li₂O-doping (0.75-6 mol%) of the investigated system followed by calcination at 600 and 800°C decreased progressively the intensity of the diffraction lines of Mn₂O₃ (Bixbyite) with subsequent increase in the lattice parameter 'a' of MgO to an extent proportional to the amount of Li₂O added. This finding might suggest that the doping process enhanced the dissolution of Mn₂O₃ in MgO forming solid solution. This treatment led also to the formation of Li₂MnO₃. Furthermore, the doping with 3 and 6 mol% Li₂O conducted at 800°C resulted in the conversion of Mn₂O₃ into Mn₃O₄, a process that took place at 1000°C in absence of Li₂O. The produced Li₂MnO₃ phase remained stable by heating at up to 1000°C. Furthermore, Li₂O doping of the investigated system at 400-1000°C resulted in a progressive measurable increase in the particle size of MgO.The catalytic activity measurements showed that the increase in the molar ratio of Mn₂O₃ in the samples precalcined at 400-800°C was accompanied by a significant increase in the catalytic activity of the treated solids. The maximum increase in the catalytic activity expressed as reaction rate constant measured at 20°C (k _20°C) attained 3.14, 2.67 and 3.25-fold for the solids precalcined at 400, 600 and 800°C, respectively. Li₂O-doping of the samples having the formula 0.1 Mn₂O₃/MgO conducted at 400-600°C brought a progressive significant increase in its catalytic activity. The maximum increase in the value of k _20°C due to Li₂O attained 1.93 and 2.75-fold for the samples preheated at 400 and 600°C, respectively and opposite effect was found for the doped samples preheated at 800°C.This revised version was published online in November 2005 with corrections to the Cover Date.     

Electron scattering and dissociative attachment by SF6 and its electrical-discharge by-products

Discrete electron-molecule processes relevant to SF₆ etching plasmas are examined. Absolute, total scattering cross sections for 0.2–12-eV electrons on SF₆, SO₂, SOF₂, SO₂F₂, SOF₄, and SF₄, as well as cross sections for negative-ion formation by attachment of electrons, have been measured. These are used to calculate dissociative-attachment rate coefficients as a function ofE/N for SF₆ by-products in SF₆.     

Synthesis, Structure, and 31P NMR of Sulfur/Oxygen-Bridged Incomplete Cubane-Type Molybdenum and Tungsten Clusters with Triphenylphosphine Ligands

Sulfur/oxygen-bridged incomplete cubane-type triphenylphosphine molybdenum and tungsten-clusters [Mo₃S₄Cl₄(H₂O)₂(PPh₃)₃]·3THF (1A), [Mo₃S₄Cl₄(H₂O)₂(PPh₃)₃]·2THF (2A), [Mo₃OS₃Cl₄(H₂O)₂(PPh₃)₃]·2THF (1B), and [W₃S₄Cl₄(H₂O)₂(PPh₃)₃]·2THF (1C) were prepared from the corresponding aqua clusters and PPh₃ in THF/MeOH. On recrystallization from THF, procedures with and without addition of hexane to the solution gave 1A and 2A, respectively, while the procedures gave no effect on the formation of 1B and 1C. Crystallographic results obtained are as follows: 1A: monoclinic, P2₁/n, a=17.141(4) Å, b=22.579(5) Å, c=19.069(4) Å, =96.18(2)°, V=7337(3) ų, Z=4, R(R _w)=0.078(0.102); 1C: monoclinic, P2 ₁/c, a=12.635(1) Å, b=20.216(4) Å, c=27.815(3) Å, =96.16(1)°, V=7062(2) ų, Z=4, R(R _w)=0.071(0.083). If the phenyl groups are ignored, the molecule [Mo₃S₄Cl₄(H₂O)₂(PPh₃)₃] in 2A has idealized CS symmetry with the mirror plane perpendicular to the plane determined by the metal atoms, while the molecule in 1A does not have the symmetry. The tungsten compound 1C is isomorphous with the molybdenum compound 2A. ³¹P NMR spectra of 1A, 2A, and 1C were obtained and compared with similar clusters with dmpe (1,2-bis(dimethylphosphino)ethane) ligands.     

Reactivity of Binary Mixtures of La(III) Oxide and Cu(II) Oxalate or Nitrate and Synthesis of La(III) Cuprate

Reactivity of mixtures of La(III) oxide and Cu(II) oxalate/nitrate in hydrated as well as anhydrous state was studied using TG, DTA and XRD. Cu(II) oxide formed in the endothermic decomposition of mixture containing hydrated Cu(II) nitrate and La(III) oxide could not form La₂CuO₄ while Cu(II) oxide formed in the exothermic decomposition of mixture containing hydrated/anhydrous Cu(II) oxalate and La(III) oxide reacts with La(III) oxide and develops the phases CuLaO₃ and La₂CuO₄. The maximum reactivity with respect to the formation of La₂CuO₄phase was observed in mixture containing anhydrous Cu(II) oxalate. This revised version was published online in July 2006 with corrections to the Cover Date.     

Synthesis of o-LiMnO2 by Microwave Irradiation and StudyIts Heat Treatment and Lithium Exchange

Microwave irradiation of a suspension of γ-MnOOH in a 4 mol dm⁻³ LiOH solution brought about a rapid formation of semicrystalline orthorhombic LiMnO₂ (o-LiMnO₂) within 30 min at 120°C. Cubic Li_1.6Mn_1.6O₄ was obtained by heating o-LiMnO₂ at 400°C; lithium could be topotactically extracted from Li_1.6Mn_1.6O₄ with acid to form cubic H_1.6Mn_1.6O₄.     

Synthesis and characterization of gallium-based perovskitetype dense membrane with oxygen semipermeability

La0.15Sr0.85Ga0.3Fe0.7O3-δ(LSGFO) and La0.15Sr0.85Co0.3Fe0.7O3-δ(LSCFO) mixed oxygen-ion and electron conducting oxides were synthesized by using a combined EDTA and citrate complexing method, and the corresponding dense membranes were fabricated. The properties of the oxide powders and membranes were characterized with combined SEM, XRD, H2-TPR, O2-TPD techniques, mechanical strength and oxygen permeation measurement. The results showed that LSGFO had much higher thermochemical stability than LSCFO due to the higher valence stability of Ga3+. After the temperature-programmed reduction by 5% H2 in Ar from 20℃to 1020℃, the basic perovskite structure of LSGFO was successfully preserved. LSGFO also favors the oxygen vacancy formation better than LSCFO. Oxygen permeation measurement demonstrated that LSGFO had higher oxygen permeation flux than LSCFO, but they had similar activation energy for oxygen transportation, with a value of 110 and 117 kJ ?mol~(-1), respectively. The difference in oxygen permeation f     

Energetics of formation of alkali and ammonium cobalt and zinc phosphate frameworks

Alkali and ammonium cobalt and zinc phosphates show extensive polymorphism. Thermal behavior, relative stabilities, and enthalpies of formation of KCoPO₄, RbCoPO₄, NH₄CoPO₄, and NH₄ZnPO₄ polymorphs are studied by differential scanning calorimetry, high-temperature oxide melt solution calorimetry, and acid solution calorimetry.α-KCoPO₄ and γ-KCoPO₄ are very similar in enthalpy. γ-KCoPO₄ slowly transforms to α-KCoPO₄ near 673 K. The high-temperature phase, β-KCoPO₄, is 5-7 kJ mol⁻¹ higher in enthalpy than α-KCoPO₄ and γ-KCoPO₄. HEX phases of NH₄CoPO₄ and NH₄ZnPO₄ are about 3 kJ mol⁻¹ lower in enthalpy than the corresponding ABW phases. There is a strong relationship between enthalpy of formation from oxides and acid-base interaction for cobalt and zinc phosphates and also for aluminosilicates with related frameworks. Cobalt and zinc phosphates exhibit similar trends in enthalpies of formation from oxides as aluminosilicates, but their enthalpies of formation from oxides are more exothermic because of their stronger acid-base interactions. Enthalpies of formation from ammonia and oxides of NH₄CoPO₄ and NH₄ZnPO₄ are similar, reflecting the similar basicity of CoO and ZnO.     

The synthesis and structural characterization of the new ternary nitrides: Ca4TiN4 and Ca5NbN5

The ternary nitrides, Ca₄TiN₄ and Ca₅NbN₅, were synthesized in sealed niobium tubes using lithium nitride as a flux at 900 and 1050 °C, respectively. The structures of both compounds were solved from single-crystal X-ray diffraction data. Ca₄TiN₄ is the first example of a calcium group IV nitride; it crystallizes in the triclinic space group (No. 2) with cell parameters a=5.9757(5) Å, b=6.0129(5) Å, c=6.0116(12) Å, α=71.565(4)°, β=79.471(4)°, γ=68.258(4)° and Z=2. Ca₄TiN₄ is isostructural with Na₄TiO₄ and contains tetrahedral TiN₄ units connected through edges and corners to CaN₄ tetrahedra and CaN₅ square pyramids. Ca₅NbN₅ crystallizes in the monoclinic space group C2/m (No. 12) with cell parameters a=11.922(7) Å, b=6.878(5) Å, c=8.936(7) Å, β=101.22(3)° and Z=4. Ca₅NbN₅ is isostructural with Ba₅NbN₅; the structure contains NbN₄ tetrahedra that share vertices with CaN₅ trigonal bipyramids.     

镥晶体的绝热量热法测试和热力学函数

文章合成了Lu(NO₃)₃(C₂H₅O₂N)_4.H₂O,用红外和元素分析对其进行了表征。用高精度全自动绝热量热仪,测定了该配合物80-382 K温区的热容, 利用实验热容数据, 根据热容与焓、熵的热力学关系, 求出了配合物85-350 K温区内每隔5 K相对于298.15K的标准热力学函数(HT - H298.15)m和(ST - S298.15)m.在80-350 K温度区间内,配合物的热容随温度升高而增大,没有相转移点和热力学吸收峰的出现,该配合物在此温度区间内是稳定存在的。     

A comparative study of CH4 and CF4 rf discharges using a consistent plasma physics and chemistry simulator

A self-consistent, one-dimensional simulator for the physics and chemistry of radio frequency (rf) plasmas was developed and applied for CH₄ and CF₄. The simulator consists of a fluid model for the discharge physics, a commercial Boltzmann equation solver for calculations of electron energy distribution fuction (EEDF), a generalized plasma chemistry code, and an interface module among the three models. The CH₄ and CF₄ discharges are compared and contrasted: CH₄ plasmas are electropositive, with negative ion densities one order of magnitude less than those of electrons, whereas CF₄ plasmas are electronegative, with ten times more negative ions than electrons. The high-energy tail of tire EEDF in CH₄, lies below both the Druyvensteyn and Maxwell distributions, whereas tire EEDF high-energy tail in CF₄ lies between the two. For CH₄, the chemistry model was applied for four species, namely, CH₄ CH₃ CH₂, and H, whereas for CF₄, five species were examined namely CF₄, CF₃, CF₂, CF, and F The predicted densities and profiles compare favorably with experimental data. Finally, the chemistry results were fedback into the physics model until convergence was obtained.