一个Yb8簇合物的合成、结构及CO2催化转化性质

使用多齿席夫碱配体H₂L与Yb(acac)₃·2H₂O反应,设计并通过溶剂热法合成了一例结构新颖的八核镱簇合物[Yb₈(acac)₄(HL)₄(L)₂(μ₃-O)₄(C₂H₅O)₄]·2C₂H₅OH·2CH₂Cl₂(1)。单晶X射线衍射分析表明,簇合物呈中心对称的八核结构,中心稀土离子Yb1(Ⅲ)为八配位的双帽三角棱柱几何构型,Yb2、Yb3和Yb4均为七配位,分别为单帽三角棱柱、五角双锥及单帽八面体几何构型。簇合物1具有良好的溶剂稳定性。近红外荧光测试表明：簇合物1在室温下表现出Yb(Ⅲ)特征发射峰。此外,催化性质研究表明：簇合物1可以有效地催化CO₂与环氧化合物的环加成反应,且作为异相催化剂表现出良好的循环性能。     

四核钬配合物的结构、慢磁驰豫行为及CO2催化转化性质

使用多齿希夫碱配体通过溶剂热的方法合成了一例新的 Ho₄配合物，即[Ho₄(NO₃)₂(acac)₄(L)₂(CH₃OH)₂]·2CH₃CN，其中H₄L=(E)-2-(羟甲基)-2-(((2-羟基萘-1-基)亚甲基)氨基)丙烷-1，3-二醇，acac=乙酰丙酮。X射线衍射分析表明，配合物呈中心对称的四核结构，中心的Ho1(Ⅲ)和Ho2(Ⅲ)均为八配位的三角十二面体几何构型。配合物1具有良好的溶剂稳定性。磁性研究表明配合物1具有慢磁弛豫行为。据我们所知，配合物1是一例少有的在零直流场下具有慢磁驰豫行为的Ho₄配合物。值得一提的是，配合物1在催化CO₂与环氧化合物的环加成反应中表现出较高的催化活性。     

两个Gd2配合物的晶体结构及磁制冷性质

使用多齿席夫碱配体（H₂L=pyridine-2-carboxylic acid （3,5-di-tert-butyl-2-hydroxy-benzylidene）-hydrazide）分别与Gd （dbm）₃·2H₂O （Hdbm=二苯甲酰基甲烷）及Gd （NO）₃·6H₂O反应,通过溶剂热法得到了2个新的Gd₂配合物[Gd₂（L）₂（dbm）₂（C₂H₅OH）₂]（1）和[Gd₂（L）₂（HL）₂（DMF）]·2CH₃CN （2）（DMF=N,N-二甲基甲酰胺）,并对其结构与磁性质进行了系统的研究。单晶结构分析表明配合物1中的每个中心Gd(Ⅲ)离子均为8配位,其配位几何构型为略微变形的三角十二面体,相邻的中心Gd(Ⅲ)离子通过2个μ₂-O连接形成了平行四边形的Gd₂O₂核心;配合物2中的每个中心Gd(Ⅲ)离子均为9配位,其配位几何构型为扭曲的球形单帽四方反棱柱,相邻的中心Gd(Ⅲ)离子通过3个μ₂-O连接形成了三角双锥形的Gd₂O₃核心。磁性测试表明配合物1和2具有磁制冷性质,其最大磁熵变（-ΔS_m）分别为20.16 J·K^-1·kg^-1（T=2.0 K,ΔH=70 kOe）和17.14 J·K^-1·kg^-1（T=2.0 K,ΔH=70 kOe）。     

基于2-硫代巴比妥酸构筑零维原子簇{[Cu6(H2tba)6]·2DMF·xSolvent}、二维层状{[Sc(H2tba)3(DMF)]·2DMF}n和三维网状{[Fe(H2tba)2(H2O)2]·2DMF}n

分别以Cu (ClO₄)₂·6H₂O、Sc (ClO₄)₃·6H₂O和Fe (ClO₄)₃·9H₂O为金属盐,2-硫代巴比妥酸(H₃tba)为配体,通过扩散反应得到了3种不同结构的配合物{[Cu₆(H₂tba)₆]·2DMF·xSolvent}(1)、{[Sc (H₂tba)₃(DMF)]·2DMF}_n(2)和[Fe (H₂tba)₂(H₂O)₂]_n(3),并用红外光谱、元素分析、热重分析和粉末X射线衍射对配合物进行了表征。单晶X射线衍射结构分析表明配合物1是一个具有三方反棱柱构型的六核铜原子簇合物,配合物2是一个具有二维层状结构的化合物,配合物3是一个具有三维网状结构的配位聚合物。配合物1在390 nm光照激发下在735 nm处有强的荧光发射峰。     

基于席夫碱配体构筑的Ln2Ⅲ配合物的结构、荧光性质及生物活性

以多齿席夫碱配体 H₂L(H₂L=(E)-N′-(3-乙氧基-2-羟基亚苄基)-3-羟基吡啶甲酰肼)为配体,与 Ln(acac)₃·2 H₂O(Ln=Tb、Ho、Er;acac^-=乙酰丙酮根)反应,通过溶剂热法,成功得到了 3例新的双核稀土配合物[Ln₂(acac)₂(L)₂(C₂H₅OH)₂](Ln=Tb (1)、Ho(2)、Er(3))。单晶X射线衍射分析表明：配合物1~3的结构主要由2个Ln^Ⅲ离子、2个乙酰丙酮根(acac^-)、2个L^2-及2个C₂H₅OH组成,中心Ln^Ⅲ离子通过2个μ₂-O原子相互连接,形成一个平行四边形的Ln₂O₂核心。固体荧光实验测试结果表明：配合物1在室温下表现出Tb^Ⅲ离子的荧光特征发射峰。此外,生物活性研究表明,与配体H₂L和稀土离子相比较,配合物1~3具有更强的抗菌活性。采用紫外光谱法、循环伏安法、凝胶电泳法和荧光光谱法研究了配合物 1~3与小牛胸腺 DNA之间的相互作用,结果表明配合物主要以插入作用的方式与小牛胸腺DNA结合。     

[Gd(C10H9N2O4)(C10H8N2O4)(H2O)3]2·phen·4H2O的晶体结构和生物活性

在水乙醇混合溶剂中，首次得到了2-羰基丙酸水杨酰腙、1，10-菲啰啉与硝酸钆形成的配合物[Gd(C₁₀H₉N₂O₄)(C₁₀H₈N₂O₄)(H₂O)₃]₂·phen·4H₂O，并测试了其单晶结构。该配合物属三斜晶系，空间群为P-1。每个配合物分子中有两个九配位的钆的结构单元，每个钆离子与两个三齿配体2-羰基丙酸水杨酰腙（分别以负一价和负二价形式）和三个水分子配位。每个钆单元在空间呈扭曲的单帽四方反棱柱。同时还有一个游离的1，10-菲啰啉存在于晶格中，通过氢键与配位水作用。生物活性试验表明该配合物对三种病原菌有一定的抑菌活性。     

铁氧簇合物[Fe11O6(OH)6(O2CCH3)15](C5H5N)6的结构和磁性质

通过三核铁盐[Fe₃O(O₂CCH₃)₆(H₂O)₃]C1在吡啶溶液中水解聚合得到铁氧簇合物[Fe₁₁O₆(OH)₆(O₂CCH₃)₁₅](C₅H₅N)₆。晶体结构表明11个铁离子(Ⅲ)中6个位于扭曲的三棱柱的顶点上，其余5个分别位于三棱柱的每个面之外。铁离子(Ⅲ)之间以氧桥或者羟基氧桥相连。变温磁化率证实铁离子(Ⅲ)之间是反铁磁耦合的。     

N，N′-(2-苯并咪唑基甲基)亚氨基甲基膦酸的双核镍化合物Ni2(bbimp)2(4，4′-bipy)(H2O)2·2H2O和Ni2(bbimp)2(H2O)2][Ni(bbimp)(H2O)2]2·4H2O

该文报道了N，N′-(2-苯并咪唑基甲基)亚氨基甲基膦酸{bbimpH₂，[(C₇H₅N₂)CH₂]₂NCH₂PO₃H₂}的2个镍化合物Ni₂(bbimp)₂(4，4′-bipy)(H₂O)₂·2H₂O (1)和[Ni₂(bbimp)₂(H₂O)₂][Ni(bbimp)(H₂O)₂]₂·4H₂O (2)。化合物1是4，4′-联吡啶作为桥连配体的中性双核结构。化合物2含有1个中性的[Ni₂(bbimp)₂(H₂O)₂]双核分子与2个中性的[Ni(bbimp)(H₂O)₂]单核分子。双核分子单元中的2个Ni(Ⅱ)离子被2个膦酸氧桥连。在化合物2中，膦酸氧桥连的2个Ni(Ⅱ)离子之间存在铁磁性相互作用。     

一个二维Honeycomb-like聚合簇合物 (Et4N)3{[MoS4Cu2(m-CN)]2(m’-CN)}·2MeCN的合成和晶体结构

采用一个预制的簇合物(Et₄N)₂[MoS₄(CuCN)₂]·H₂O(1)和HAc在MeCN中混合反应，生成了一个有趣的二维聚合簇合物(Et₄N)₃{[MoS₄Cu₂(m-CN)]₂(m’-CN)}·2MeCN (2)。通过元素分析，红外光谱及单晶X-射线衍射分析对簇合物2进行了表征。在2的结构中，前驱体1中的MoS₄Cu₂簇核得到了保留，并且此簇核作为三重连接点通过单一氰桥和其他相同的簇核相连，形成一个阴离子型的2D (6,3)（蜂窝状）网络。由预制的簇合物1通过醋酸诱导形成的超分子2表明这种简单的合成方法有可能应用到许多其他相关的体系。     

基于柔性配体的双核铽配位聚合物[Tb2(tda)3(H2O)2]的合成、晶体结构和荧光性质

在水热条件下,利用硫代羟基二乙酸配体[thiodiglycolic acid=H₂tda]和TbCl₃·nH₂O合成了新型稀土配合物[Tb₂(tda)₃(H₂O)₂]。单晶结构表明,配合物是以共边多面体[Tb₂O₁₆]为基本单元构筑的二维结构,并通过弱相互作用拓展为三维超分子体系。中心原子铽与氧原子的配位数是8和9,分别形成了单帽反四棱柱和三帽三角棱柱构型的空间配位多面体。配体H₂tda在配合物中存在两种配位模式：(a) 双“顺-顺桥式双齿、螯合桥式三齿”模式和(b) 双“螯合双齿、顺-反桥式双齿”模式。荧光光谱研究表明：该配合物在室温下呈现较强的绿色荧光发射。配合物属三斜晶系,空间群P1。     

Synthesis and properties of the double perovskites La2NiVO6, La2CoVO6, and La2CoTiO6

The double perovskites La₂CoVO₆, La₂CoTiO₆, and La₂NiVO₆, are described. Rietveld fitting of neutron and powder X-ray diffraction data show La₂NiVO₆ and La₂CoVO₆ to have a disordered arrangement of B-cations whereas La₂CoTiO₆ shows ordering of the B-cations (with ∼5% Co/Ti inversion). Curie-Weiss fits to the linear region of the 1/χ plots reveal Weiss temperatures of −107, −34.8, and 16.3 K for La₂CoVO₆, La₂CoTiO₆, and La₂NiVO₆, respectively, and magnetic transitions are observed. La₂CoTiO₆ prepared by our method differs from material prepared by lower-temperature routes. A simple antiferromagnetic spin model is consistent with the data for La₂CoTiO₆. These compounds are semiconductors with bandgaps of 0.41 (La₂CoVO₆), 1.02 (La₂CoTiO₆) and 0.45 eV (La₂NiVO₆).     

Synthesis, crystal structure, infrared and Raman spectra of Sr4Cu3(AsO4)2(AsO3OH)4·3H2O and Ba2Cu4(AsO4)2(AsO3OH)3

The two new compounds, Sr₄Cu₃(AsO₄)₂(AsO₃OH)₄·3H₂O (1) and Ba₂Cu₄(AsO₄)₂(AsO₃OH)₃(2), were synthesized under hydrothermal conditions. They represent previously unknown structure types and are the first compounds synthesized in the systems SrO/BaO-CuO-As₂O₅-H₂O. Their crystal structures were determined by single-crystal X-ray diffraction [space group C2/c, a=18.536(4) Å, b=5.179(1) Å, c=24.898(5) Å, β=93.67(3)°, V=2344.0(8) Å³, Z=4 for 1; space group P4₂/n, a=7.775(1) Å, c=13.698(3) Å, V=828.1(2) Å³, Z=2 for 2]. The crystal structure of 1 is related to a group of compounds formed by Cu²⁺-(XO₄)³⁻ layers (X=P⁵⁺, As⁵⁺) linked by M cations (M=alkali, alkaline earth, Pb²⁺, or Ag⁺) and partly by hydrogen bonds. In 1, worth mentioning is the very short hydrogen bond length, D···A=2.477(3) Å. It is one of the examples of extremely short hydrogen bonds, where the donor and acceptor are crystallographically different. Compound 2 represents a layered structure consisting of Cu₂O₈ centrosymmetric dimers crosslinked by As1φ₄ tetrahedra, where φ is O or OH, which are interconnected by Ba, As2 and hydrogen bonds to form a three-dimensional network. The layers are formed by Cu₂O₈ centrosymmetric dimers of CuO₅ edge-sharing polyhedra, crosslinked by As1O₄ tetrahedra. Vibrational spectra (FTIR and Raman) of both compounds are described. The spectroscopic manifestation of the very short hydrogen bond in 1, and ABC-like spectra in 2 were discussed.     

Cr2(WO4)3和Cr2(MoO4)3的负热膨胀特性研究

用液相反应-前驱物烧结法制备了Cr₂(WO₄)₃和Cr₂(MoO₄)₃粉体。298～1 073 K的原位粉末X射线衍射数据表明Cr₂(WO₄)₃和Cr₂(MoO₄)₃的晶胞体积随温度的升高而增大, 本征线热膨胀系数分别为(1.274±0.003)×10^-6 K^-1和(1.612±0.003)×10^-6 K^-1。用热膨胀仪研究了Cr₂(WO₄)₃和Cr₂(MoO₄)₃在静态空气中298～1 073 K范围内热膨胀行为，即开始表现为正热膨胀，随后在相转变点达到最大值，最后表现为负热膨胀，其负热膨胀系数分别为(-7.033±0.014)×10^-6 K^-1和(-9.282±0.019)×10^-6 K^-1。     

Ni-P-Zn3(PO4)2(ZnSnO3、ZnSiO3)纳米复合化学镀层性质和组成的研究

研究了温度、时间、浓度等对Ａ３钢片上Ｎi-P-Zn3(PO4)2、Ni-P-ZnSnO3和Ｎi-P-ZiSiO3纳米复合合化学镀层外貌的影响,用扫描电子显微镜（ＳＥＭ）观察外貌、称重法测定厚度;通过１０％ＮaCl溶液、１％Ｈ２Ｓ气体加速腐蚀试验,１０％ＣuSO4溶液点滴试验等多种手段测定其耐腐蚀性能,用Ｘ－射线光电子谱（ＸＰＳ）及俄歇电子能谱（ＳＥＳ）测定其价态组成,结果表明：在最佳施镀条件下,可得光亮、致密、耐腐蚀性强于Ａ３钢、磷化膜及Ｎi-P镀层的纳米复合化学镀层,镀层的原子百分组成约为（％）：Ｎi-P-Zn3(PO4)2:Ni70.00,P12.47,Zn3(PO4)213.93,C3.6;Ni-P-ZnSnO3;Ni77.56,P10.00,ZnSnO39.84,C2.6;Ni-P-NiSiO3,Ni83.00,P10.96,ZnSi5.15,C0.89.     

Non-centrosymmetric Ba3Ti3O6(BO3)2

The compound previously reported as Ba₂Ti₂B₂O₉ has been reformulated as Ba₃Ti₃B₂O₁₂, or Ba₃Ti₃O₆(BO₃)₂, a new barium titanium oxoborate. Small single crystals have been recovered from a melt with a composition of BaTiO₃:BaTiB₂O₆ (molar ratio) cooled between 1100°C and 850°C. The crystal structure has been determined by X-ray diffraction: hexagonal system, non-centrosymmetric space group, a=8.7377(11) Å, c=3.9147(8) Å, Z=1, wR(F²)=0.039 for 504 unique reflections. Ba₃Ti₃O₆(BO₃)₂ is isostructural with K₃Ta₃O₆(BO₃)₂. Preliminary measurements of nonlinear optical properties on microcrystalline samples show that the second harmonic generation efficiency of Ba₃Ti₃O₆(BO₃)₂ is equal to 95% of that of LiNbO₃.     

Crystal growth, structural characterization and magnetic properties of Ca3CuRhO6, Ca3Co1.34Rh0.66O6 and Ca3FeRhO6

Single crystals of Ca₃CuRhO₆, Ca₃Co_1.34Rh_0.66O₆ and Ca₃FeRhO₆ were synthesized by high temperature flux growth in molten K₂CO₃ and structurally characterized by single crystal X-ray diffraction. While Ca₃Co_1.34Rh_0.66O₆ and Ca₃FeRhO₆ crystallize with trigonal (rhombohedral) symmetry in the space group , Z=6: Ca₃Co_1.34Rh_0.66O₆a=9.161(1) Å, c=10.601(2) Å; Ca₃FeRhO₆a=9.1884(3) Å, c=10.7750(4) Å; Ca₃CuRhO₆ adopts a monoclinic distortion of the K₄CdCl₆ structure in the space group C2/c, Z=4: a=9.004(2) Å, b=9.218(2) Å, c=6.453(1) Å, β=91.672(5). All crystals of Ca₃CuRhO₆ examined were twinned by pseudo-merohedry. Ca₃CuRhO₆, Ca₃Co_1.34Rh_0.66O₆, and Ca₃FeRhO₆ are structurally related and contain infinite one-dimensional chains of alternating face-sharing RhO₆ octahedra and MO₆ trigonal prisms. In the monoclinic modification, the copper atoms are displaced from the center of the trigonal prism toward one of the rectangular faces adopting a pseudo-square planar configuration. The magnetic properties of Ca₃CuRhO₆, Ca₃Co_1.34Rh_0.66O₆, and Ca₃FeRhO₆ are discussed.     

Multianvil high-pressure/high-temperature preparation, crystal structure, and properties of the new oxoborates Dy4B6O14(OH)2 and Ho4B6O14(OH)2

This paper reports about two new hydrogen-containing rare-earth oxoborates RE₄B₆O₁₄(OH)₂ (RE=Dy, Ho) synthesized under high-pressure/high-temperature conditions from the corresponding rare-earth oxides, boron oxide, and water using a Walker-type multianvil equipment at 8 GPa and 880 °C. The single crystal structure determination of Dy₄B₆O₁₄(OH)₂ showed: Pbcn, a=1292.7(2), b=437.1(2), , Z=2, R1=0.0190, and wR2=0.0349 (all data). The isotypic holmium species revealed: Pbcn, a=1292.8(2), b=436.2(2), , Z=2, R1=0.0206, and wR2=0.0406 (all data). The compounds exhibit a new type of structure, which is built up from layers of condensed BO₄-tetrahedra. Between the layers, the rare-earth cations are coordinated by 7+2 oxygen atoms. Furthermore, we report about temperature-resolved in situ powder diffraction measurements, DTA/TG, and IR-spectroscopic investigations into RE₄B₆O₁₄(OH)₂ (RE=Dy, Ho).     

一维纳米Co_3O_4,Ag/Co_3O_4及CuO/Co_3O_4的合成与电催化性能(英文)

采用水热合成法制备了Co3O4及复合Ag/Co3O4、CuO/Co3O4一维纳米产品。用XRD,FE-SEM和TEM手段对产品进行了表征。采用循环伏安法研究了合成产品修饰的玻碳电极在碱性溶液中对对硝基苯酚的电催化还原性能。与裸玻碳电极相比,1mmol·L-1的对硝基苯酚在用Co3O4、特别是CuO/Co3O4修饰的玻碳电极上还原的峰电流明显增大,用Ag/Co3O4(Ag/Co原子比分别为1∶5和2∶5)修饰的玻碳电极催化还原对硝基苯酚时,尽管还原峰电流增大不是太大,但其峰电位明显降低(分别降低0.265和0.371V)。     

Conversion of NO in NO/N2, NO/O2/N2, NO/C2H4/N2 and NO/C2H4/O2/N2 Systems by Dielectric Barrier Discharge Plasmas

An experimental study on the conversion of NO in the NO/N₂, NO/O₂/N₂, NO/C₂H₄/N₂ and NO/C₂H₄/O₂/N₂ systems has been carried out using dielectric barrier discharge (DBD) plasmas at atmospheric pressure. In the NO/N₂ system, NO decomposition to N₂ and O₂ is the dominating reaction; NO conversion to NO₂ is less significant. O₂ produced from NO decomposition was detected by an on-line mass spectrometer. With the increase of NO initial concentration, the concentration of O₂ produced decreases at 298 K, but slightly increases at 523 K. In the NO/O₂/N₂ system, NO is mainly oxidized to NO₂, but NO conversion becomes very low at 523 K and over 1.6% of O₂. In the NO/C₂H₄/N₂ system, NO is reduced to N₂ with about the same NO conversion as that in the NO/N₂ system but without NO₂ formation. In the NO/C₂H₄/O₂/N₂ system, the oxidation of NO to NO₂ is dramatically promoted. At 523 K, with the increase of the energy density, NO conversion increases rapidly first, and then almost stabilizes at 93–91% of NO conversion with 61–55% of NO₂ selectivity in the energy density range of 317–550 J L⁻¹. It finally decreases gradually at high energy density. A negligible amount of N₂O is formed in the above four systems. Of the four systems studied, NO conversion and NO₂ selectivity of the NO/C₂H₄/O₂/N₂ system are the highest, and NO/O₂/C₂H₄/N₂ system has the lowest electrical energy consumption per NO molecule converted.     

Sol-gel synthesis of K3InF6 and structural characterization of K2InC10O10H6F9, K3InC12O14H4F18 and K3InC12O12F18

K₃InF₆ is synthesized by a sol-gel route starting from indium and potassium acetates dissolved in isopropanol in the stoichiometry 1:3, with trifluoroacetic acid as fluorinating agent. The crystal structures of the organic precursors were solved by X-ray diffraction methods on single crystals. Three organic compounds were isolated and identified: K₂InC₁₀O₁₀H₆F₉, K₃InC₁₂O₁₄H₄F₁₈ and K₃InC₁₂O₁₂F₁₈. The first one, deficient in potassium in comparison with the initial stoichiometry, is unstable. In its crystal structure, acetate as well as trifluoroacetate anions are coordinated to the indium atom. The two other precursors are obtained, respectively, by quick and slow evaporation of the solution. They correspond to the final organic compounds, which give K₃InF₆ by decomposition at high temperature. The crystal structure of K₃InC₁₂O₁₄H₄F₁₈ is characterized by complex anions [In(CF₃COO)₄(OH_x)₂]^(5−2x)− and isolated [CF₃COOH_2−x]^(x−1)− molecules with x=2 or 1, surrounded by K⁺ cations. The crystal structure of K₃InC₁₂O₁₂F₁₈ is only constituted by complex anions [In(CF₃COO)₆]³⁻ and K⁺ cations. For all these compounds, potassium cations ensure only the electroneutrality of the structure. IR spectra of K₂InC₁₀O₁₀H₆F₉ and K₃InC₁₂O₁₂F₁₈ were also performed at room temperature on pulverized crystals.