四溴代对苯二甲酸根及二吡啶基丙烷构筑的锌(Ⅱ)及镉(Ⅱ)配位聚合物的合成及晶体结构

在室温和甲醇/水溶液为溶剂的条件下,以四溴代对苯二甲酸(H2TBTA)及1,3-二(4-吡啶基)丙烷(BPP)为配体合成了[Zn(TBTA)(BPP)]n(1)和[Cd(TBTA)(BPP)2(H2O)2]n(2)2个配位聚合物,对其进行了X-射线单晶衍射、元素分析、红外光谱分析和热重等性质表征。结果表明:配合物1为二维(2D)层状网络结构;配合物2为一维(1D)链状结构;H2TBTA配体中的羧基都采取单齿模式与金属离子配位;配合物中的氢键作用对其结构的稳定性起关键作用。     

四溴代对苯二甲酸及2，2′-联吡啶构筑的铜配位聚合物的合成、晶体结构及热稳定性

以四溴代对苯二甲酸(H2TBTA)与2,2′-联吡啶(2,2′-bipy)为配体,与硝酸铜在水和甲醇混合溶剂中合成了1个一维铜配合物{[Cu(2,2′-bipy)(TBTA)(H2O)].H2O}n,并通过元素分析、红外分析、热重分析、X-射线粉末衍射和X-射线单晶衍射对其进行了表征。该配合物属于正交晶系,空间群为Pna21,a=1.399 9(11)nm,b=0.929 3(7)nm,c=1.557 9(11)nm,V=2.027(3)nm3,Z=4,R1=0.053 5。中心Cu(Ⅱ)离子处于一个五配位环境中,且在配合物中存在着π-π相互作用和氢键作用。热重分析表明该配合物在203℃开始发生分解。     

四溴代对苯二甲酸根及二吡啶基丙烷构筑的锌(Ⅱ)及镉(Ⅱ)配位聚合物的合成及晶体结构

在室温和甲醇/水溶液为溶剂的条件下,以四溴代对苯二甲酸(H₂TBTA)及1,3-二(4-吡啶基)丙烷(BPP)为配体合成了[Zn(TBTA)(BPP)]_n (1)和[Cd(TBTA)(BPP)₂(H₂O)₂]_n(2)2个配位聚合物,对其进行了X-射线单晶衍射、元素分析、红外光谱分析和热重等性质表征。结果表明:配合物1为二维(2D)层状网络结构;配合物2为一维(1D)链状结构;H₂TBTA配体中的羧基都采取单齿模式与金属离子配位;配合物中的氢键作用对其结构的稳定性起关键作用。     

3,5-二(2',5'-苯二羧酸)苯甲酸构筑的金属有机配合物的荧光识别及磁性

设计合成了3种新颖的金属有机配合物（MOCs）：{[Pb₂（HL）（phen）]·2H₂O}_n（1）,{[Ni（H₃L）（4,4''-bipy）_1.5（H₂O）₄]·6H₂O}_n（2）和{[Ni₂（HL）（1,4-bibb）（H₂O）]·（CH₃CN）·H₂O}_n（3）（H₅L=3,5-二（2'',5''-苯二羧酸）苯甲酸,phen=1,10-菲咯啉,4,4''-bipy=4,4''-联吡啶,1,4-bibb=1,4-二（苯并咪唑）苯）,并通过单晶X射线衍射、红外光谱（IR）、热重分析（TG）和粉末衍射对它们进行结构表征。结构分析表明1是基于[Pb₂（μ₂-COO）₂（μ₁-COO）₄]SBUs的一维链状结构;2是二维层状结构,其拓扑符号为{4.6²}₂{4².6².8²};3是一个3D网络结构,其拓扑符号为{6².8⁴}{6⁴.8²}₂。进一步研究了配合物荧光和磁性能。荧光检测显示,配合物1在水溶液中可以高灵敏识别Fe³⁺和Cr₂O₇^2-离子。同时研究了配合物1对Fe³⁺和Cr₂O₇^2-猝灭机理。磁性分析表明配合物3中的Ni（Ⅱ）离子之间存在反铁磁相互作用。     

High pressure electrical transport behavior in SrF_2 nanoplates

The charge transport behavior of strontium fluoride nanocrystals has been investigated by in situ impedance measurement up to 35 GPa.It was found that the parameters changed discontinuously at each phase transition.The charge carriers in SrF_2 nanocrystals include both F~-ions and electrons.In the Fm3 m phase,pressure makes the electronic transport easier,while makes it more difficult in the Pnma phase.The defects at grain boundaries dominate the electronic transport process.Pressure could make the charge-discharge processes in the Fm3 m phase much easier,but make it more difficult in the Pnma phase.     

High-Pressure Phase Transition in Cyclo-octane

Structural behaviour of cyclo-octane under high pressure is studied by using a synchrotron x-ray source in a diamond anvil cell （DAC） up to 40.2 GPa at room temperature. The cyclo-octane firstly solidifies to the triclinic phase at 0.87 GPa. With the increasing pressure, the phase of cyclo-octane changes to the tetragonal phase at about 6.0 GPa and then transforms to amorphous phase above 18.2 GPa, which is kept till to 40.2 GPa. All the phase transitions of cyclo-octane are irreversible.     

直流电弧自催化合成β-SiC纳米线

采用C,Si和SiO₂为反应原料,利用直流电弧法制备出长直的β-SiC纳米线。纳米线的直径为100～200 nm,长度为10～20 μm,并且沿着<111>方向生长。通过X射线衍射(XRD)、扫描电子显微术(SEM)、透射电子显微术(TEM)、拉曼光谱等手段,对β-SiC纳米线进行表征。探讨了β-SiC纳米线自催化气-液-固(VLS)生长机制。     

Structural Phase Transformations of ZnS Nanocrystalline Under High Pressure

In-situ energy dispersive x-ray diffraction on ZnS nanocrystalline was carried out under high pressure by using a diamond anvil cell. Phase transition of wurtzite of 10nm ZnS to rocksalt occurred at 16.0GPa, which was higher than that of the bulk materials. The structures of ZnS nanocrystalline at different pressures were built by using materials studio and the bulk modulus, and the pressure derivative of ZnS nanocrystalline were derived by fitting the equation of Birch-Murnaghan. The resulting modulus was higher than that of the corresponding bulk material, which indicates that the nanomaterial has higher hardness than its bulk materials.