富氮杂环配位超分子化合物的合成、结构及光谱特征

以2,6-二(5-甲基-1H-吡唑-3-基)吡啶(简写为H2L)为第一配体,以均苯四甲酸和乙酸为第二配体,合成了2个新的配位超分子化合物[Ni(H2L)2]·(Me O-H2BTA)2(1)和Mn(H2L)(Ac)2(2)(H4BTA∶均苯四甲酸,HAc∶乙酸),并由元素分析、红外光谱、紫外-可见光谱以及X射线单晶衍射等对其进行了表征,分析了其光谱及结构特征。晶体结构分析表明,化合物1属于正交晶系,Pbcn空间群,a=0.95747(8)nm,b=1.99273(13)nm,c=2.50175(13)nm,α=90°,β=90°,γ=90°,V=4.773 3(6)nm3,Z=4;化合物2属于单斜晶系,Cc空间群,a=1.11300(13)nm,b=2.0239(2)nm,c=0.97308(12)nm,α=90°,β=118.555(16)°,γ=90°,V=1.9253(4)nm3,Z=4。     

含吡唑基的1,5-苯并硫氮杂衍生物的合成及晶体结构

以1-苯基-3-甲基-5-苯氧基-吡唑-4-甲醛和1-苯基-3-甲基-5-对甲苯氧基-吡唑-4-甲醛为原料,在碱性条件下与苯乙酮(取代苯乙酮)发生羟醛缩合,合成出10种新型含吡唑基的查尔酮;再用此查尔酮与邻氨基硫酚在冰醋酸中反应,合成了10种新的1,5-苯并硫氮杂,化合物的结构经元素分析、IR和1HNMR确认,同时测定了化合物6c的晶体结构.化合物6c属单斜晶系(Monoclinic),空间群P2(1)/n,晶胞参数a=1.1793(2)nm,b=1.1907(2)nm,c=1.8726(4)nm,α=90°,β=104.71(3)°,γ=90°,M=522.04,V=2.5432(9)nm3,D=1.363Mg/m3,Z=4,F(000)=1088.     

类杯[6]芳烃修饰的多酸基超分子化合物的合成与晶体结构

利用水热合成方法合成了1个新型类杯芳烃修饰的Keggin型超分子化合物Ag6L6(PMo12O40)2(1)(L=5-甲基四氮唑),其中6个5-甲基四氮唑配体和6个银配位形成了类杯[6]芳烃的多核银配合物.通过红外光谱、元素分析和X射线单晶衍射方法确定了该化合物的晶体结构.单晶结构分析表明化合物1属于六方晶系,R-3空间群,晶胞参数a=1.779 0 8(8)nm,b=1.779 0 8(8)nm,c=2.408 8 5(19)nm,α=90°,β=90°,γ=120°,V=6.602 8(7)nm3,Z=3.     

一维Z形链状吡啶三唑-Zn(Ⅱ)化合物的合成、晶体结构及荧光性能

通过水热法成功合成了一例一维"Z"形链状结构的化合物[(4,3′-Hbpt)_2Zn(adp)]_n(1)(4,3′-Hbpt=3-(4-吡啶基)-5-(3-吡啶基)-1-H-1,2,4-三唑;adp=己二酸离子)),并通过X射线单晶衍射、元素分析、X射线粉末衍射和荧光光谱等方法对该化合物进行了结构表征和性质研究.X射线单晶衍射分析表明,化合物1属于单斜晶系,C2/c空间群,晶胞参数为a=1.938 8 nm,b=0.877 6 nm,c=1.844 1 nm,α=90°,β=109.1°,γ=90°,V=2.965 0 nm~3,D_c=1.470 g/cm~3,Z=4,F(000)=1 352,GOOF=0.957.在化合物1中,Zn~(2+)离子通过己二酸桥接形成一维"Z"形链状结构.此外,通过荧光光谱对化合物1的荧光性质进行了研究.     

苯并咪唑类化合物一步法合成及表征

采用对甲氧基苯甲醛、对羟基苯甲醛和邻苯二胺直接关环合成了1-(对甲氧基苄基)-2-(对甲氧基苯基)-苯并咪唑、1-(对羟基苄基)-2-(对羟基苯基)-苯并咪唑化合物.通过元素分析、IR、核磁分析对它们进行了表征,并培养了1-(对甲氧基苄基)-2-(对甲氧基苯基)-苯并咪唑化合物晶体.该晶体经X射线衍射确定为正交晶系,空间群Pna2(1),a=2.0194(7)nm,b=1.5657(4)nm,c=0.5498(1)nm,α=90°,β=90°,γ=90°,V=1.7383(8)nm3,Z=4,Mr=344.40,Dc=1.316g/cm3,μ=0.85 cm-1,F(000)=728.     

芳醛缩N-(2-乙胺)-9,10-二氢蒽-9,10-桥-α,β-琥珀酰亚胺Schiff碱衍生物的合成及晶体结构

合成了2个N-(2-乙胺)-9,10-二氢蒽-9,10-桥-α,β-琥珀酰亚胺希夫碱衍生物,利用单晶X-射线衍射法测定了它们的晶体结构.化合物1为正交晶系,Pca21空间群,晶胞参数a=1.132 59(15)nm,b=2.535 6(4)nm,c=0.835 82(12)nm;α=90.00°,β=90.00°,γ=90.00°,V=2.4003(6)nm3,Z=4;化合物2为三斜晶系,P-1空间群,晶胞参数a=1.012 9(15)nm,b=1.190 1(16)nm,c=1.307 5(18)nm;α=67.17(3)°,β=72.88(3)°,γ=75.41(3)°,V=1.371(3)nm3,Z=2.     

一种新型双缩合螺吡喃的合成、表征及晶体结构

以过量吲哚啉和5-硝基水杨醛为原料合成了4-(2-亚甲基-1-乙基-3,3-二甲基吲哚啉-2'-基)-6-硝基-1'-乙基-3',3'-二甲基-螺[3,4-二氢-2H-l-苯并吡喃-2,2'-吲哚啉],通过核磁共振、红外光谱、元素分析对其结构进行了表征.同时利用X单晶衍射仪测定了该化合物的结构,结果表明:晶体属单斜晶系,空间群P21/n,a=1.2476(3)nm,b=1.1939(2)nm,c=2.0317(4)nm,α=90°,β=107.45(3)°,γ=90°,Dc=1.205g/cm3,μ=0.077mm-1,F(000)=1120,V=2.8871(10)nm3,Z=4.     

N,N,N,N-四乙酰氧甲基-1,5-二苯基-2,4,6,8-四氮杂双环[3.3.0]-3,7-辛二酮的合成及晶体结构研究

以苯基苷脲为原料设计合成N,N,N,N-四乙酰氧甲基-1,5-二苯基-2,4,6,8-四氮杂双环[3.3.0]-3,7-辛二酮,并对其结构进行了X-单晶衍射表征.结果表明:该化合物晶体属于单斜晶系,空间群,P_(21/n),a=1.102 3(7)nm,b=1.741 3(11)nm,c=1.261 2(8)nm,α=90°,β=99.601(17)°,γ=90°,V=2.386 88 nm~3,Z=4,R(1)=0.075 9.量子化学计算结果表明,化合物的偶极矩为1.530×10~(-29) C·m.     

超声辐射下2-氨基-7-甲基-4-芳基-5-氧代-4-H,5H吡喃并[4,3-b]吡喃-3-腈的“一锅法”合成

以芳醛、丙二腈与6-甲基-4-羟基-2-吡喃酮为原料,醋酸酐为溶剂,超声辐射下一步合成了2-氨基-7-甲基-4-芳基-5-氧代-4H, 5H-吡喃并[4,3-b]吡喃-3-腈系列产物.产率达72%～83%.产物结构经红外光谱、核磁共振和元素分析测试技术表征.其中化合物4e的结构经单晶X射线衍射进一步确证,单晶体属单斜晶系,空间群C2/c,晶胞参数:A=2.14917(7)nm, b=0.82498(2)nm, c=1.79137(6)nm, α=90°, β=112.104(2)°, γ=90°, Mr=314.72, V=2.94254(16)nm3, Z=8, Dc=1.421kg/m3, F(000)=1296, R=0.0495, wR=0.0878.     

三个基于3-(2,5-二羧基苯基)-吡啶羧酸的Cu(Ⅱ)、Mn(Ⅱ)配合物的结构及磁性

通过水热法合成了3个新型配位聚合物:[Cu(Hdppa)(H_2O)]_n(1)、{[Cu_2(dppa)(μ_2-OH)(H_2O)]·H_2O}_n(2)和{[Mn_3(dppa)_2(H_2O)_4]·2H_2O}_n(3),(H3dppa=3-(2,5-二羧基苯基)-吡啶羧酸),并对其进行了元素分析、红外光谱、粉末X射线衍射和热重分析表征。X射线单晶衍射分析结果表明:化合物1属于单斜晶系,P21/c空间群,a=1.371(2)nm,b=0.805(11)nm,c=1.266(19)nm,β=112.74(3)°,Z=4;化合物2属于三斜晶系,P1空间群,a=0.839(4)nm,b=1.039(5)nm,c=1.110(5)nm,α=98.31°,β=110.630(3)°,γ=111.90(3)°,Z=2;化合物3属于三斜晶系,P1空间群,a=0.881(6)nm,b=0.939(6)nm,c=1.038(7)nm,α=100.29°,β=97.990(10)°,γ=111.13(7)°,Z=1。化合物1以配体Hdppa2-桥联Cu(Ⅱ)形成一维链状结构;化合物2和3以配体dppa3-分别桥联Cu(Ⅱ)和Mn(Ⅱ)形成二维层状结构,并进一步通过氢键形成三维超分子结构。变温磁化率研究表明在化合物1和化合物2中存在较强的铁磁耦合作用,其磁交换常数分别为4.44和8.94 cm-1;而化合物3中Mn(Ⅱ)离子之间存在反铁磁相互作用。     

Phase relations in the K2W2O7-K2WO4-KPO3-Bi2O3 system and structure of K6.5Bi2.5W4P6O34

The phase relations in the cross-section of the K₂W₂O₇-K₂WO₄-KPO₃ containing 15 mol% Bi₂O₃ were undertaken using flux method. Crystallization fields of K_6.5Bi_2.5W₄P₆O₃₄, K₂Bi(PO₄)(WO₄), Bi₂WO₆, KBi(WO₄)₂ and their cocrystallization areas were identified. Novel phase K_6.5Bi_2.5W₄P₆O₃₄ was characterized by single-crystal X-ray diffraction: sp. gr. P−1, a=9.4170(5), b=9.7166(4), c=17.6050(7) Å, α=90.052(5)°, β=103.880(5)° and γ=90.125(5)°. It has a layered structure, which contains {K₇Bi₅W₈P₁₂O₆₈}_∞ layers stacked parallel to ab plane and sheets composed by potassium atoms separating these layers. Sandwich-like {K₇Bi₅W₈P₁₂O₆₈}_∞ layers are assembled from [W₂P₂O₁₃]_∞ and [BiPO₄]_∞ building units, and are penetrated by tunnels with K/Bi atoms inside. FTIR-spectra of K₂Bi(PO₄)(WO₄) and K_6.5Bi_2.5W₄P₆O₃₄ were discussed on the basis of factor group theory.     

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.     

KCl-KBO2-K2CO3, K2MoO4-KBO2-K2CO3, and K2WO4-KBO2-K2CO3 ternary systems

phase diagrams of KCl-KBO₂-K₂CO₃, K₂MoO₄-KBO₂-K₂CO₃, and K₂WO₄-KBO₂-K₂CO₃ ternary systems were studied by a calculation-experimental method and differential thermal analysis (DTA). The coordinates of ternary eutectics were determined to be E ₁: 622°C, 8.5 mol % KBO₂, 56.5 mol % KCl, and 35 mol % K₂CO₃; E ₂: 710°C, 23 mol % KBO₂, 43 mol % K₂CO₃, and 34 mol % K₂MoO₄; E ₃: 710°C, 23 mol % KBO₂, 43 mol % K₂CO₃, and 34 mol % K₂WO₄. The specific heats of melting of the eutectics were determined.     

Li2SO4-Na2SO4-H2O和Li2SO4- K2SO4-H2O溶液的体积性质

本文用高精度数字式振荡管密度计测定了288K至318K温度范围内Li₂SO₄ + Na₂SO₄ + H₂O和 Li₂SO₄ + K₂SO₄ + H₂O三元体系的密度。混合溶液的离子强度范围从0.1到4.5 mol.kg_–1,混合溶液中Na₂SO₄和K₂SO₄的离子强度分数为0.2,0.4,0.6和0.8。用密度实验值拟合得到了不同温度下Pitzer离子相互作用模型混合参数θ_V和 ψ_V,模型的计算值与实验值的偏差在±0.002 g.cm_–3以内。用Pitzer模型计算了不同离子强度下三元体系的混合体积。     

Solubility in the Na2Cr2O7-(NH4)2Cr2O7-K2Cr2O7-H2O system

Solubility in the Na₂Cr₂O₇-(NH₄)₂Cr₂O₇-K₂Cr₂O₇-H₂O four-component water-salt system at 25, 50, and 75°C was studied for the first time. Phase field boundaries for individual salts and potassium and ammonium dichromate solid solutions, monovariant lines, and invariant points were determined. Experimental data were used to optimize the looped isohydric process of potassium dichromate preparation involving additional salts.     

NaBO2-NaCl-Na2CO3, NaBO2- Na2CO3-NaMoO4, NaBO2- Na2CO3-NaWO4, and NaBO2-NaCl-Na2WO4 ternary systems

The phase diagrams of the NaBO₂-NaCl-Na₂CO₃, NaBO₂-Na₂CO₃-Na₂MoO₄, NaBO₂- Na₂CO₃-Na₂WO₄, and NaBO₂-NaCl-Na₂WO₄ ternary systems were studied by a calculation-experimental method and differential thermal analysis. The coordinates of ternary eutectics were determined: E ₁: 612°C, 16 mol % NaBO₂, 42 mol % NaCl, and 42 mol % Na₂CO₃; E ₂: 568°C, 12 mol % NaBO₂, 28 mol % Na₂CO₃, and 60 mol % Na₂MoO₄; E ₃: 575°C, 12 mol % NaBO₂, 32 mol % Na₂CO₃, and 56 mol % Na₂WO₄; E ₄: 628°C, 8 mol % NaBO₂, 20 mol % NaCl, and 72 mol % Na₂WO₄; and E ₅: 655°C, 9 mol % NaBO₂, 53 mol % NaCl, and 38 mol % Na₂WO₄.     

Extension of the La7Mo7O30 structural type with La7Nb3W4O30 and La7Ta3W4O30 compounds

Two compounds of formula La₇A₃W₄O₃₀ (with A=Nb and Ta) were prepared by solid-state reaction at 1450 and 1490 °C. They crystallize in the rhombohedric space group R-3 (No. 148), with the hexagonal parameters: , and , . The structure of the materials was analyzed from X-ray, neutron and electronic diffraction. These oxides are isostructural of the reduced molybdenum compound La₇Mo₇O₃₀, which are formed of perovskite rod along [111]. An order between (Nb, Ta) and W is observed.     

Theoretical study of polyoxide clusters B20O30, Al20O30, V20O50, Si20O30H20, and Si20O30F20

The structural, electronic, and vibrational characteristics and energies of the isolated polyoxide clusters B₂₀O₃₀, Al₂₀O₃₀, V₂₀O₅₀, Si₂₀O₃₀H₂₀, and Si₂₀O₃₀F₂₀ and their complexes with the H⁻ ion and ammonia complexes Al₂₀O₃₀ · nNH₃ have been calculated by the density functional theory B3LYP method with different basis sets. The computation results show that the symmetric closo structure I _h with oxygen bridges located above the centers of the faces of an empty [M₂₀] dodecahedron is more favorable for V₂₀O₅₀, Si₂₀O₃₀H₂₀, and Si₂₀O₃₀F₂₀. For B₂₀O₃₀, the cage closo isomer is also more favorable than the other isomers, but its structure is severely distorted as compared to a dodecahedron and has a symmetry close to C ₃ . For Al₂₀O₃₀, the I _h structure corresponds to a high-lying local minimum of the potential energy surface. For Al₂₀O₃₀, a set of unusual puckshaped isomers of symmetry C _i , with different numbers of four-coordinate atoms ^IVAl and three-coordinate atoms ^IIIO, was localized; these structures are more than 90 kcal/mol more favorable than the dodecahedron I _h . The most favorable isomer of Al₂₀O₃₀ contains twelve four-coordinate atoms ^IVAl and four five-coordinate atoms ^VAl. The energies of dissociation of the most favorable M₂₀O₃₀ clusters into the M₂O₃ (C _2v ) and M₄O₆ (T _d ) fragments and, in the case of Al₂₀O₃₀, also into the Al₈O₁₂ (O _h ) and Al₁₂O₁₈ (D _3d ) fragments, have been estimated. The conclusion has been drawn that these clusters can, in principle, exist and can be experimentally detected in the isolated state. Analogous calculations have been performed for ammonia complexes Al₂₀O₃₀ · nNH₃ with n varying from 1 to 20. The effect of solvation on the relative stability of the dodecahedral and puckshaped isomers of the Al₂₀O₃₀ cluster is observed. The isomers with ammonia molecules in their first coordination sphere become much closer to one another on the energy scale; however, the dodecahedron remains a considerably less favorable intermediate. Original Russian Text ? O.P. Charkin, N.M. Klimenko, D.O. Charkin, 2008, published in Zhurnal Neorganicheskoi Khimii, 2008, Vol. 53, No. 4, pp. 624–635.     

Li2O-TiO2-SiO2-P2O5和Li2O-TiO2-Al2O3-P2O5体系锂离子固体电解质的制备及性能研究

一些具有NASICON型网格结构的固体电解质具有高的电导率和好的稳定性,NASICON的意思是Na Super Ionic Conductor[1]。当NaZr2(PO4)3中P5 被Si4 部分取代时便可以得到具有NASICON结构的Na1 xZr2SixP3-xO12体系,其具有高的钠离子电导率。然而有相同结构的Li1 xZr2SixP3-xO12体系的离子电导率却很低,这是因为Li 半径太小,而NASICON三维网格结构的离子通道太大,两者不匹配而使电导率下降[2]。但当LiZr2(PO4)3中Zr4 被离子半径小些的Ti4 取代,所得LiTi2(PO4)3的通道就与Li 半径相匹配,适合于锂离子的迁移,从而使其电导率…     

Structural chemistry of Sr3Cr2WO9, Ca3Cr2WO9, and Ba3Cr2WO9

We have studied the preparation and crystallographic structure of three perovskite-type compounds: Sr₃Cr₂WO₉, cubic, the lattice parameter of which is a = 7.812Å; Ca₃Cr₂WO₉, tetragonal, the lattice parameters of which are a = 5.408 Å and c = 7.635Å; and Ba₃Cr₂WO₉, hexagonal, the lattice parameters of which are a = 5.691 Å and c = 13.957Å. We have compared these three structures and shown the relationship between the dimensions of the alkaline-earth metal and the existence of the different structures.