层状结构钒磷酸盐(pipzH2)2[(VO)3(HPO4)2(PO4)2]·H2O的水热合成及热稳定性研究

水热合成了钒磷酸盐体系中少有的结构中具有多面体共棱连接的层状孔道结构化合物(pipzH2)2[(VO)3(HPO4)2(PO4)2]·H2O的纯相.用ICP、单晶XRD、TG-DTA、粉晶XRD和SEM对产物进行了表征.结果表明,化合物在空气中开始失重的温度为274 ℃,随着温度的升高,化合物中有机分子分解,同时伴随着重结晶过程,但晶体的外观形貌保持不变直至有机部分分解殆尽.相变过程分析和与模板相同的(pipzH2)0.5[(VO)(PO4)]的热稳定性对比研究表明,有机模板的稳定性及分解过程不但影响化合物的热稳定性和热变化过程,还影响原晶体微形貌的保持;无机骨架结合的牢固程度在很大程度上影响化合物的热稳定性.     

孔道结构钒铝磷酸盐(NH3CH2CH2NH2)[(VO)Al(PO4)2]的水热合成及热稳定性

用XRD,TG-DTA,FT-IR和SEM对水热法合成的孔道结构钒铝磷酸盐(NH3CH2CH2NH2)[(VO)Al(PO4)2]进行了热性能表征.该化合物中有机组份的分解温度,在氧化气氛中为305～529℃,在惰性气氛中为411～593℃.有机组分的分解逸出导致了结构的破坏,但晶体的微形貌没有发生明显的变化;温度继续升高,发生相变.该化合物热稳定性较其它含有机模板的孔道结构钒磷酸盐要高,主要原因在于结构中存在[AlO4]和[PO4]共顶连接而成的一维链,这种链增加了骨架的强度.     

层状结构钒磷酸盐（pipzH2）2[（VO）3（HPO4）2（PO4）2]·H2O的水热合成及热稳定性研究

水热合成了钒磷酸盐体系中少有的结构中具有多面体共棱连接的层状孔道结构化合物（pipzH2）2[（VO）3（HPO4）2（PO4）2]·H20的纯相。用ICP、单晶XRD、TG-DTA、粉晶XRD和SEM对产物进行了表征。结果表明，化合物在空气中开始失重的温度为274℃，随着温度的升高，化合物中有机分子分解，同时伴随着重结晶过程，但晶体的外观形貌保持不变直至有机部分分解殆尽。相变过程分析和与模板相同的（pipzH2）0.5[（VO）（PO4）]的热稳定性对比研究表明，有机模板的稳定性及分解过程不但影响化合物的热稳定性和热变化过程，还影响原晶体微形貌的保持；无机骨架结合的牢固程度在很大程度上影响化合物的热稳定性。     

孔道结构铁磷酸盐(C4H12N2)2[Fe6(HPO4)2(PO4)6(H2O)2]·H2O的水热合成及热变化过程研究

在与前人不同的条件下水热合成了孔道结构铁磷酸盐(C4H12N2)2[Fe6(HPO4)2(PO4)6(H2O)2]·H2O.用ICP、有机元素分析仪、TG-DTA、变温XRD、变温FT-IR等分析技术对其成份、物相和热变化过程进行了系统研究.结果表明,室温-330℃,化合物失去吸附水,有机模板哌嗪开始氧化脱氢;330-380℃,哌嗪环破坏,大部分有机模板和结晶水脱除,化合物结构骨架明显破坏;470℃化合物完全非晶化;650℃形成FePO4和Fe4(P2O7)3新物相.哌嗪起到平衡电荷和支撑结构的作用.哌嗪环破坏并脱除是导致结构破坏的根本原因.     

孔道结构铁磷酸盐（C4H12N2）2[Fe6（HPO4）2（PO4）6（H2O）2]·H2O的水热合成及热变化过程研究

在与前人不同的条件下水热合成了孔道结构铁磷酸盐（C4H12N2）2[Fe6（HPO4）2（PO4）6（H2O）2]·H2O。用ICP、有机元素分析仪、TG-DTA、变温XRD、变温FT-IR等分析技术对其成份、物相和热变化过程进行了系统研究。结果表明,室温～330℃,化合物失去吸附水,有机模板哌嗪开始氧化脱氢;330～380℃,哌嗪环破坏,大部分有机模板和结晶水脱除,化合物结构骨架明显破坏;470℃化合物完全非晶化;650℃形成FePO4和Fe4（P2O7）3新物相。哌嗪起到平衡电荷和支撑结构的作用。哌嗪环破坏并脱除是导致结构破坏的根本原因。     

新型磷酸钒孔道结构化合物(H3NCH2CH2NH3)3[(VO)4(PO4)2(HPO4)4]的表征及热性能研究

利用五氧化二钒、磷酸作前驱物,乙二胺作模板,水热法合成了新型孔道结构磷酸盐化合物(H3NCH2CH2NH3)3[(VO)4(PO4)2(HPO4)4].借助红外光谱(FT-IR)、热分析(TG-DTA)、粉晶X 射线衍射(XRD)及扫描电镜(SEM)等手段,对该化合物晶体在受热条件下的孔容脱除、结构变化及热相变特征等进行了系统研究.从晶体化学角度对其成分、结构及热稳定性之间的关系进行了探讨.指出应通过优化模板、元素替代等方法减弱模板分子与无机骨架间的键联强度及改善基本结构骨架的牢固性,进一步提高其热稳定性.     

三维孔道结构钒磷酸盐[H3N(CH2)3NH3]2[H3N(CH2)3NH2][H2N(CH2)3NH2]-[V(H2O)2(VO)8(OH)4(PO4)4(HPO4)4]·4H2O的水热合成和结构表征

以1,3-丙二胺为模板,水热合成了三维孔道结构钒磷酸盐[H3N(CH2)3NH3]2[H3N(CH2)3NH2][H2N(CH2)3NH2][V(H2O)2(VO)8(OH)4(PO4)4(HPO4)4]·4H2O(DAP-V9P8).用单晶X射线衍射、红外光谱和热重法对该化合物的晶体结构进行了表征.DAP-V9P8的无机骨架由[VO5]、[VO6]、[PO4]和[HPO4]通过共顶点连接而成.孔道中充填的丙二胺分子随所处结晶学位置不同,有三种完全不同的分子构象.其中,位于//b轴直径达1.82nm椭圆形孔道中心的丙二胺分子碳链呈独特的直线状分布.晶体学参数:a=1.4820(9)nm,b=1.0255(4)nm,c=1.8181(9)nm,β=90.391(8)°;P21/n(No.14);R1=0.0772,wR2=0.2004(I＞(2σI)).与等结构的其它化合物进行了系统的结构比较.     

三维孔道结构(H_3NCH_2CH_2NH_3)_2(H_3NCH_2CH_2NH_2)[V~Ⅲ(H_2O)_2(V~ⅣO)_8(OH)_4(H(P,B)O_4)_4(P,B)O_4)_4(H_2O)_2]·3H_2O的水热合成及晶体化学研究——(1)水热合成与产物表征

为了探讨化学成份对VPO体系孔道结构化合物结构稳定性的影响,根据酸碱平衡原理进行了合成实验设计;利用V2O5、H3PO4、H3BO3 等简单的无机前驱物、乙二胺作结构导向剂,水热法合成了孔道结构钒硼磷酸盐化合物(H3NCH2CH2NH3 )2 (H3NCH2CH2NH2 ) [VⅢ (H2O)2 (VⅣO)8 (OH)4 (H(P,B)O4 )4 ( (P,B)O4 )4 (H2O)2 ]·3H2O(简称V9 (P,B)8 en)。典型的反应起始物摩尔比为n(V2O5 ):n(H3BO3 ):n(H3PO4 ):n(en):n(H2O) =0. 89:3. 50: 3. 50: 3. 60: 265(pH值为 6. 5),在 175℃、自生压力条件下恒温晶化 6. 5d(最终pH值为 5. 9 )。通过电子探针、粉末X射线衍射、红外吸收光谱、原子占位度修正等方法,对产物的化学成份、物相及其结构等进行了实验研究。证实V9 (P,B)8 en为V9P8 en的类质同象化合物,不同晶粒中B与P的含量有差别,B与P之比为 0. 1: 7. 9~2. 54: 5. 46(原子比),但恒有V: (P+B)≈9: 8。表明通过合理设计和控制合成条件,可在保持V9P8 en基本结构不变的前提下通过同晶取代引入新的化学成份,并由此探讨成份与结构稳定性的关系。     

三维孔道结构(H3NCH2CH2NH3)2(H3NCH2CH2NH2)[VⅢ(H2O)2(VⅣO)8(OH)4(H(P,B)O4)4(P,B)O4)4(H2O)2]·3H2O的水热合成及晶体化学研究——(1)水热合成与产物表征

为了探讨化学成份对VPO体系孔道结构化合物结构稳定性的影响,根据酸碱平衡原理进行了合成实验设计;利用V2O5、H3PO4、H3BO3等简单的无机前驱物、乙二胺作结构导向剂,水热法合成了孔道结构钒硼磷酸盐化合物(H3NCH2CH2NH3)2(H3NCH2CH2NH2)[VⅢ(H2O)2(VⅣO)8(OH)4(H(P,B)O4)4((P,B)O4)4(H2O)2]·3H2O(简称V9(P,B)8-en).典型的反应起始物摩尔比为n(V2O5):n(H3BO3):n(H3PO4):n(en):n(H2O)=0.89:3.50:3.50:3.60:265(pH值为6.5),在175℃、自生压力条件下恒温晶化6.5d(最终pH值为5.9).通过电子探针、粉末X射线衍射、红外吸收光谱、原子占位度修正等方法,对产物的化学成份、物相及其结构等进行了实验研究.证实V9(P,B)8-en为V9P8-en的类质同象化合物,不同晶粒中B与P的含量有差别,B与P之比为O.1:7.9～2.54:5.46(原子比),但恒有V:(P+B)≈9:8.表明通过合理设计和控制合成条件,可在保持V9P8-en基本结构不变的前提下通过同晶取代引入新的化学成份,并由此探讨成份与结构稳定性的关系.     

晶体(NH4)2C4H4O6:VO2+的EPR参量及局域结构的研究

采用叠加模型和双旋-轨耦合参量模型,建立了结构参数与EPR参量之间的定量关系;较好地解释了[VO(H2O)5]2+络离子的局域结构和EPR参量;研究结果发现,(NH4)2C4H4O6:VO2+晶体中络离子[VO(H2O)5]2+的键长为R//≈0.130nm,R⊥≈0.195nm;在(NH4)2C4H4O6:VO2+晶体中,局域结构沿C4轴方向呈压缩的八面体结构;所得EPR参量的理论计算与实验测量数据符合很好.     

Vibrational Studies of Gel Grown Ferroelectric RbHC4H4O6 and SrC4H4O6 4H2O Crystals

Single crystals of Rubidium Hydrogen Tartrate (RbHT) and Strontium Tartrate Tetrahydrate (SrTT) have been grown by a gel technique using a chemical reaction method. A controlled reaction has been employed between tartaric acid and feed solution (RbCl for RbHT and Sr(NO₃)₂) at room temperature. The laser Raman and FT-IR spectra of these crystals are recorded in the frequency range 100 - 4000 cm^-1. The presence of tartrate ion, monohydrogen tartrate ion, water molecules and external mode vibrational frequencies are identified and discused. The doublet and broad nature of tartrate ion vibrational frequencies have also been observed and analysed.     

The Study of Phase Equilibria in the Cs2SO4–Rb2SO4–H2SO4–H2O System

Crystallography Reports - The phase equilibria in the quaternary water–salt system Cs2SO4–Rb2SO4–H2SO4–H2O have been studied. The crystallization ranges are determined, and...     

Synthesis and crystal structure of [Tb4(H2O)2](C2O4)2(C5H6O4)4

A terbium complex associating two ligands, oxalate and glutarate, was prepared under hydrothermal conditions at 200°C by treating an aqueous suspension of terbium oxalate decahydrate with glutaric acid and guanidinium carbonate. Its structure was solved by X-ray diffraction on a single crystal. It crystallizes in the monoclinic space group P2₁ with lattice constants, a = 9.514(1) Å, b = 9.0681(8) Å, c = 19.702(2) Å, and = 97.90(1)°. The terbium atoms and the oxalate ligands build dense chains which are connected by one side of the carboxylic group of some glutarate ligands, thus forming a sheet at the c level 0 and 1/2. These sheets are bridged by glutarate groups. The terbium atoms are ninefold coordinate with nine oxygen atoms of the ligands or with one water molecule and eight oxygen atoms of the ligands. Each polyhedron of the terbium atoms share one edge and one face of oxygen atoms with the two neighboring ones. The oxalate ligands are bischelating and bismonodentate. The coordination scheme of glutarate differs: either they are bismonodentate from one side and chelating and monodentate from the other side or they are chelating and monodentate from both sides.     

Production of Complex Hydrosulphates in the K3H(SO4)2–Rb3H(SO4)2 Series: II. Phase Equilibria in the K2SO4–Rb2SO4–H2SO4–H2O System

Crystallography Reports - The phase equilibria in the K2SO4–Rb2SO4–H2SO4–H2O system have been investigated under isothermal conditions at 25°C. The concentration limits of...     

Electronic Structure of [Cu(C7H4NO3S)2(H2O)4] · 2H2O Crystal

The electronic absorption spectrum and ESR spectrum of the crystal of the title compound [Cu(C₇H₄NO₃S)₂(H₂O)₄] · 2 H₂O, are measured. The experimental results are discussed quantitatively by using the ligand field theory and the radial wave function of non-free Cu(II). The electronic structure of the compound is in agreement with its crystal structure.     

Characterisation of the Six-coordinated Octahedral Site in Cd(C4H2O4) · 2H2O Crystals

Optical absorption spectra of Co(II) and Ni(II) doped cadmium maleate dihydrate (CMDH) are recorded at room temperature and liquid nitrogen temperature. The UV–VIS–NIR spectra are characteristic of the transition metal ions in solids. The results and analyses of the spectra indicate near octahedral site symmetry for cobalt ion and trigonally distorted octahedral site symmetry for nickel ion. The following crystal field parameters are derived. The IR spectra are characteristic of the host lattice CMDH.     

Deformation-induced After-Glow in [(C2H5)4N]2MnBr4 Crystals

The mechanoluminescence appears in [(C₂H₅)₄N]₂MnBr₄ crystals even after their mechanical deformation. During the excitation of mechanoluminescence by the impact of a piston on to the crystals, the peak corresponding to the mechanoluminescence intensity versus time curve and the total intensity of mechanoluminescence increase with the impact velocity and decrease with the temperature of the crystals. It seems that the electric field produced during the inpact of the piston on to the crystal may perturb the ground and excited states of the molecules comprising the crystals. Thus the mechanoluminescence may follow the rate of compression during the deformation of the crystal and it may decay with the decay rate of phosphorescence after the compression. The mechanoluminescence and high pressure photoluminescence spectra are also reported.