无铅和稀土的大尺寸分子基绿光荧光晶体:(C5H13ClN)2[MnCl4]

通过氯化锰和2-二甲氨基异丙基氯盐酸盐在溶液中的反应,制备了一类绿光分子基晶态材料：（C₅H₁₃ClN）₂[MnCl₄]（1）。该材料在紫外光激发后发出强烈的绿色荧光,并且热分析测试表明其具有较好的热稳定性（分解温度大于450 K）。结构和光谱分析表明其优异的光学性能归因于[MnX₄]^2-四面体中Mn²⁺的⁴T₁（G）→⁶A₁电子跃迁。     

有机杂化硫代碲酸盐化合物（H2en）TeS3和[Ni（en）3]TeS3的溶剂热合成与表征

用低温溶剂热法合成了2种分立结构的有机杂化硫代碲（Ⅳ）酸盐化合物（H₂en）TeS₃（1）和[Ni（en）₃]TeS₃（2）（en=乙二胺）,通过X-射线单晶衍射,红外光谱,元素分析等手段对它们的结构进行了表征。晶体结构解析结果表明：2个化合物均属单斜晶系,空间群分别为P2₁和P2₁/c。化合物1和2具有孤立三角锥[TeS₃]^2-阴离子,化合物1的平衡阳离子为双质子化乙二胺[H₂en]²⁺,阴离子基团[TeS₃]^2-和阳离子基团[H₂en]²⁺之间通过N-H…S氢键连接。化合物2的阳离子基团为过渡金属Ni与乙二胺的配合物[Ni（en）₃]²⁺。另外,对该2种晶体进行了紫外-可见漫反射光谱测试和热重分析。     

两个基于[SMo12O40]2-和冠醚基超分子阳离子的无机-有机杂化晶体的合成及晶体结构

以18-冠-6和4-碘-苯铵盐,二苯并30-冠-10和3-氟-4-氯-苯铵盐为超分子阳离子构建单元,分别引入到Keggin型[SMo₁₂O₄₀]^2-中,使用H管扩散法和溶剂挥发法合成了无机-有机杂化材料[（4-I-Anis）（[18]crown-6）]₂[SMo₁₂O₄₀]·CH₃CN（1）和[（3-F-4-Cl-Anis）₂（DB[30]crown-10）][SMo₁₂O₄₀]·2CH₃CN（2）（4-I-Anis=4-碘-苯铵盐;3-F-4-Cl-Anis=3-氟-4-甲基苯铵盐;DB[30]crown-10=二苯并30-冠-10）。通过红外光谱、元素分析、热重分析、固态漫反射光谱和X射线单晶结构分析对化合物进行了表征。结构分析表明,晶体1和2通过非共价键自组装作用构建而成,冠醚基超分子阳离子是通过N-H…O氢键作用形成。晶体1中,在bc平面,每个[SMo₁₂O₄₀]^2-多酸阴离子被6个超分子阳离子（4-I-Anis）（[18]crown-6）围绕,形成六边形的结构;晶体2中,在bc平面,每个[SMo₁₂O₄₀]^2-多酸阴离子被4个大的超分子阳离子（3-F-4-Cl-Anis）₂（DB[30]crown-10）围绕,形成四边形的结构。热重分析表明,氢键在维持晶体1和2的稳定性上起着主要的作用。固态漫反射光谱表明,[SMo₁₂O₄₀]^2-和冠醚基超分子阳离子之间存在电荷转移作用。     

两个具stp三维拓扑构型的稀土配位聚合物{[Ln2（pda）3（H2O）2]2H2O}n（Ln=Nd/La）

本文利用水热合成方法,将稀土氧化物与邻苯二乙酸（H₂pda）反应得到了2个新颖的稀土配位聚合物{[Ln₂（pda）₃（H₂O）₂]·2H₂O}_n（Ln=Nd（1）,La（2））。测定了它们的晶体结构,并进行了X-射线单晶衍射、红外光谱、荧光光谱和热重分析等性质的表征。晶体结构测定表明这2个化合物为异质同晶化合物。属单斜晶系,C2/c空间群。晶体学参数分别为配合物1：a=2.62906（18）nm,b=1.61172（11）nm,c=0.78327（5）nm,β=93.173（5）°,V=3.3139（4）nm³,Z=4,F（000）=1840,μ=3.173mm^-1,D_c=1.878g·cm^-3,R₁=0.0226,wR₂=0.0609;配合物2：a=2.6271（14）nm,b=1.6149（8）nm,c=0.7966（4）nm,β=92.850（9）,V=3.375（3）nm³,Z=4,F（000）=1816,μ=2.570mm^-1,D_c=1.823g·cm^-3,R₁=0.0466,wR₂=0.1416。化合物中邻苯二乙酸配体连接相邻的稀土金属离子,形成复杂的具有stp拓朴构型的三维网络结构。     

两例具有大磁滞的氰根桥联{FeⅢ2NiⅡ}单链磁体

我们利用具有不同对称性的同分异构体,通过改变分子间氢键网络,操控单链磁体行为,成功合成了2例化合物：[Ni^Ⅱ（L1）][Fe^Ⅲ（Tp）（CN）₃]₂·3.5H₂O （1）和[Ni^Ⅱ（L2）][Fe^Ⅲ（Tp）（CN）₃]₂·3H₂O （2）,其中Tp=hydrotris （pyrazolyl） borate,L1=3,4-bis （1H-imid-azol-1-yl） thiophen,L2=1,2-bis （1H-imidazol-1-yl） thiophen）。磁性研究表明,1和2表现为具有不同矫顽场的单链磁体行为。1的矫顽场为8.41 kOe,而2的矫顽场为3.84 kOe。     

基于[LnMo12]二十面体的三维稀土钼酸盐骨架的合成、结构及荧光性能

通过缓慢蒸发溶剂法合成了2例新的三维稀土钼酸盐：[Ln （H₂O）₃]₃[LnMo₁₂O₄₂]·xH₂O,其中Ln=Eu （1）、Tb （2）,x=7（1）,10.17（2）。这2种稀土钼酸盐中都含有新颖的二十面体[LnMo₁₂O₄₂]构建单元,该单元通过与{LnO₉}多面体进一步连接形成三维网络。光致发光测试表明,化合物1和2显示出明显不同的发射特征,这与Eu³⁺和Tb³⁺离子的不同能级跃迁密切相关。化合物1表现出较强的红色发射（CIE色度坐标为（0.66,0.33））、高发光强度、较大的荧光量子产率（约60%）,对应于从⁵D₀到⁷F_J （J=4、3、2、1、0）的跃迁;化合物2表现出浅绿色发射（CIE色度坐标为（0.34,0.60））,对应从⁵D₄到⁷F_J （J=6、5、4、3）的能级跃迁,其发光强度较弱和荧光量子产率较低（约20%）。有趣的是,一定量的Tb³⁺引入和大量溶剂分子的存在导致化合物2发生部分荧光猝灭,但对化合物1的荧光几乎没有影响。     

氰基桥联的Fe2Ni2单分子磁体的合成与磁性

利用三氰基构筑单元Bu₄N[Fe^Ⅲ（PzTp）（CN）₃]（PzTp=tetrakis（pyrazolyl）borate）和4,4''-二甲氧基-2,2''-联吡啶（4,4''-dmobpy）配体,合成了2例氰基桥联的Fe^Ⅲ₂Ni^Ⅱ₂四核配合物。单晶X射线衍射表明化合物[Fe^Ⅲ（PzTp）（CN）₃]₂[Ni^Ⅱ₂（4,4''-dmobpy）₄][Fe^Ⅲ（PzTp）（CN）₃]₂·2CH₃OH（1）和[Fe^Ⅲ（PzTp）（CN）₃]₂[Ni^Ⅱ₂（4,4''-dmobpy）₄]（PF₆）₂（2）具有四核四方形分子结构。直流磁化率测试表明配合物1和2均表现为分子内的铁磁耦合作用。交流磁化率测试表明配合物1和2在零场下具有慢磁弛豫行为,有效能垒分别为12.8和13.0 K。     

蝎型铜配合物：Cu2[ μ-pz]2[HB(pz)3]2和Cu[B(pz)4]2的合成、结构及热分解动力学性质

本文设计合成了两种以聚吡唑硼酸盐、吡唑为配体的铜配合物Cu₂[ μ-pz]₂[HB(pz)₃]₂(1)和Cu[B(pz)₄]₂(2)(pz：吡唑(C₃H₄N₂))。运用元素分析、红外光谱对配合物进行了表征，并用X-ray衍射测定了它们的晶体结构。非等温热分解动力学研究表明：配合物1的热分解反应分两步，配合物2的热分解反应一步进行。通过计算，配合物1热分解的第一步反应的可能机理为成核与生长，n=1/4；第二步反应的可能机理为化学反应。其非等温动力学方程分别为：dα/dT=A/β e^-E/RT·1/4(1-α)[-ln(1-α)]^-3和dα/dT=A/β e^-E/RT·(1-α)²。分解反应的表观活化能分别是520.37 kJ·mol^-1和149.65 kJ·mol^-1；指前因子lnA分别是118.06 s^-1和28.10 s^-1。配合物2热分解的可能机理为化学反应。其非等温动力学方程为：dα/dT=A/β e^-E/RT·(1-α)²。分解反应的表观活化能是111.41 kJ·mol^-1；指前因子lnA是21.20 s^-1。     

无机-有机杂化硫属化合物[Mn（1，2-dap）2（H2O）]2（μ-Sn2Q6）（Q=S、Se）和[Mn（tren）]2（μ-Sn2S6）的合成、晶体结构与性能

采用溶剂热方法合成了3个多元硫属化合物[Mn（1,2-dap）₂（H₂O）]₂（μ-Sn₂Q₆）（Q=S（1）和Se（2））和[Mn（tren）]₂（μ-Sn₂S₆）（3）,用X-射线单晶衍射测定了化合物的结构,并通过红外光谱、紫外-可见漫反射光谱对其进行了表征。单晶结构解析表明,化合物1和2都属于正交晶系,Pccn空间群（No.56）,晶体结构是由[Mn（1,2-dap）₂（H₂O）]²⁺配合物阳离子和[Sn₂Q₆]^4-二聚体通过Mn-Q键连接而成的[Mn（1,2-dap）₂（H₂O）]₂（μ-Sn₂Q₆）低聚体,相邻的低聚体之间通过氢键相连形成三维结构。化合物3属于三斜晶系,晶体结构是由[Mn（tren）]₂（μ-Sn₂S₆）单元通过氢键连接而成的二维结构。紫外-可见漫反射光谱结果显示化合物1,2和3的带隙分别为2.5,2.1,2.4eV,属于半导体材料。     

基于PbBr2的有机-无机杂化化合物的合成和晶体结构

合成得到了2个新的有机-无机杂化化合物{（4-CH₃-Bz-4-Ph-Py）[PbBr₃]}_n（1）（4-CH₃-Bz-4-Ph-Py⁺=4-甲基苄基-4-苯基吡啶离子）和{（4-F-Bz-4-Ph-Py）[PbBr₃]}_n（2）（4-F-Bz-4-Ph-Py⁺=4-氟苄基-4-苯基吡啶离子）。对化合物1和2进行了元素分析、粉末X射线衍射等表征,并利用X射线单晶衍射测定了它们的单晶结构,配合物1与2同构,均属于正交晶系,P2₁2₁2空间群。结构研究表明,配合物1和2中,铅溴八面体通过共边连接方式,形成[Pb₃Br₉]_n三链,有机阳离子填充在无机溴化铅链空隙中。配合物1和2均未作手性分离。     

Crystal structure of KSbP2O8

KSbP₂O₈ crystallizes in the rhombohedral system, space group $\text{R}\text{3}$, with a = 4.7623(4) Å, c = 25.409(4)Å, and Z = 3. The structure was determined from 487 reflexions collected on a NONIUS CAD4 automatic diffractometer with MoK^?α radiation. The final R index and weighted R_w index are 0.030 and 0.038, respectively. This structure is built up from layers of SbO₆ octahedra and PO₄ tetrahedra sharing corners. These (SbP₂O^?₈)_n layers are very similar to the (ZrP₂O^2?₈)_n layers in the well-known α-ZrP compound.     

Crystal structures of V3S4 and V5S8

Crystal structures of the ordered phases of V₃S₄ and V₅S₈ were refined with single crystal data. Both are monoclinic. Chemical compositions, space groups and lattice constants are as follows: VS_1.47, $\text{I2}\text{m}$ (No. 12), a = 5.831(1), b = 3.267(1), c = 11.317(2)Å, β = 91.78(1)° and VS_1.64, $\text{F}\text{2}\text{m}$ (No. 12), a = 11.396(11), b = 6.645(7), c = 11.293(4), Å, β = 91.45(6)°. In both structures, short metal-metal bonds were found between the layers as well as within them. In comparison with the structure of Fe₇S₈, the stability of NiAs-type structure was discussed based on the detailed metal-sulfur distances.     

Crystal structure of binary molybdate Pr2Hf3(MoO4)9

Crystals of binary praseodymium and hafnium molybdate of Pr₂Hf₃(MoO₄)₉ composition are grown by solution-melt crystallization under spontaneous nucleation conditions. By the X-ray diffraction data (X8 Apex automated diffractometer, MoK _α radiation, 2262 F(hkl), R = 0.0170) its composition and crystal structure are determined. Parameters of the trigonal unit cell are: a = b = 9.8001(1) ? c = 58.7095(8) ?, V = 4883.15(10) ?³, Z = 6, space group R c. The crystal structure is composed of three types of polyhedra: MoO₄ tetrahedra, HfO₆ octahedra, and nine-vertex PrO₉. All three types of polyhedra are bonded among themselves by common oxygen vertices of bridging MoO₄ tetrahedra forming an openwork three-dimensional structure. Original Russian Text Copyright ? 2009 by B. G. Bazarov, V. G. Grossman, R. F. Klevtsova, A. G. Anshits, T. A. Vereshchagina, L. A. Glinskaya, Yu. L. Tushinova, K. N. Fedorov, and Zh. G. Bazarova __________ Translated from Zhurnal Strukturnoi Khimii, Vol. 50, No. 3, pp. 587–590, May–June, 2009.     

Crystal structure of [Cu(NH3)4](ReO4)2

At T = 150 K, the crystal structure of [Cu(NH₃)₄](ReO₄)₂ is studied: a = 6.5167(3) ?, b = 6.7790(3) ?, c = 7.4627(3) ?, α = 67.336(1)°, β = 80.004(1)°, γ = 70.687(1)°, V = 286.70(2) ?³, P-1 space group, Z = 1, d _x = 3.661 g/cm³. We analyze the packing of ions using the translation sublattice isolation technique.     

Crystal structure of Fe2P2O7

Fe₂P₂O₇ crystallizes in the $\text{C}\text{1}$ space group with lattice parameters a = 6.649(2)Å, b = 8.484(2)Å, c = 4.488(1)Å, α = 90.04°, β = 103.89(3)°, γ = 92.82(3)°, and ?_cal = 3.86 g/cc. It is essentially isostructural with β-Zn₂P₂O₇. As in the Zn compound, the bridging oxygen atom in the P₂O₇ group shows a high anisotropic thermal motion. It appears that the P-O-P bond angle is linear as a result of extensive π bonding with the p orbitals on the bridging oxygen atom. The high thermal motion is vibration of the atom into cavities in the structure.     

Crystal growth and electrical conduction of PbMoO4 and PbWO4

The phenomenon of the coloration of Czochralski grown single crystals of PbMoO₄ and PbWO₄ is discussed. This coloration is supposed to be related to an intrinsic point defect. We propose that during the crystal growth a loss of oxygen occurs, and consequently, oxygen deficient crystals are produced. The existence of electronic charge carriers at high temperatures and ionic majority defects in the oxygen sublattice is confirmed by conductivity measurements. The color center is supposed to be an oxygen vacancy that has trapped one or two electrons. On the basis of this simple model, various aspects of the coloration can be understood.     

Crystal structures and magnetic properties of BaTiF5 and CaTiF5

Single crystals of BaTiF₅ and CaTiF₅ were obtained by the Czochralski and Bridgman techniques, respectively. The crystal structures were determined by X-ray diffraction; BaTiF₅: $\text{14}\text{m}\text{, a = 15.091(5)}$Å, c = 7.670(3)Å; CaTiF₅: $\text{I2}\text{c}\text{, a = 9.080(4)}$Å, b = 6.614Å, c = 7.696(3)Å, β = 115.16(3)°. Both structures are characterized by the presence of either branched or straight chains of TiF₆ octahedra. BaTiF₅ contains the unusual dimeric unit (Ti₂F₁₀)^4?. Magnetic susceptibility measurements were performed on both compounds in the temperature range 4.2 to 300 K, however, no evidence for magnetic interactions between the Ti³⁺ moments were observed.     

Crystal structure of α-AlB12

The crystal structure of α-AlB₁₂ (tetragonal; a = 10.158(2) Å, c = 14.270(5) Å, space group P4₁2₁2 or P4₃2₁2) has been determined by the single-crystal X-ray diffraction method. It was solved by the Fourier technique initially based on a partial B₁₂ icosahedral structure, which was inferred from crystal chemical considerations. Refinement was made with the aid of a full-matrix least-squares program leading to a final R value of 3.0%. The structure is based on a three-dimensional framework consisting of B₁₂ icosahedra, B₁₉ units, and single B atoms; the B₁₉ unit is a twinned icosahedron with a triangular composition plane and a vacant apex on each side. The chemical unit is Al_3.2·2B₁₂·B·B₁₉ and its number in the unit cell is 4. The Al atoms are distributed statistically over five sites in the boron framework. The occupancies of the sites are 72, 49, 24, 15, and 2%, respectively.     

Crystal data and phase transitions of KLiWO4 and KLiMoO4

Crystal data and phase transitions of KLiWO₄ and KLiMoO₄ were investigated using a high-temperature X-ray powder diffractometer. Phase transitions were observed at 350°C for KLiWO₄ and at 360°C for KLiMoO₄. It was found that the room temperature phases were isostructural with stuffed derivatives of tridymite and the high-temperature phases were isostructural with stuffed derivatives of cristobalite.