立方晶型Sb2O3纳米晶的合成及光催化性能

采用沉淀法合成了立方晶型Sb2O3纳米晶,通过X射线衍射(XRD)、扫描电镜(SEM)、透射电镜(TEM)、紫外-可见漫反射光谱(UV-Vis DRS)和电子自旋共振谱(ESR)等对样品进行了详细的表征。以紫外光光催化降解甲基橙为反应模型评价了样品的光催化性能。结果表明:沉淀法合成的立方晶型Sb2O3纳米晶颗粒小,表现出良好的光催化性能。对立方晶型Sb2O3纳米晶光催化降解甲基橙的原因进行了探讨,并提出了降解甲基橙的反应机理。     

金红石型TiO2的快速晶型转变

SnO2;金红石型TiO2的快速晶型转变     

尼龙-6 18的晶型转变研究

以偶偶尼龙-6 18为例, 通过示差扫描量热分析(DSC), 广角X射线衍射(WAXD)与傅里叶变换红外光谱(FTIR)等方法研究了其Brill转变的过程, 探索了脂肪族聚酰胺的晶型转变的本质. X射线衍射结果表明， 随着温度的升高, 尼龙-6 18由三斜晶系转变为假六方晶型, 同时其DSC曲线上出现一个较宽的吸热峰. 红外光谱结果表明, 在其晶型转变过程中, 晶体内氢键强度逐渐减弱, 与酰胺键相连的C—C和C—N键发生扭曲. 酰胺基团之间的亚甲基链段的振动逐渐增强, 部分亚甲基单元由反式构象变成旁式构象, 最后整齐排列的亚甲基链段逐渐变得无序化.     

尼龙1216晶型转变的红外光谱研究

采用变温红外光谱研究了尼龙1216的Brill转变并测得Brill温度约为150℃。一些α谱带在转变过程中消失，氢键强度也急剧减弱。这些现象证明了Brill转变的“局部熔融”机理。     

SnCl4对纳米二氧化钛晶相结构的低温转变控制研究

采用二种方法制备了低温下晶相结构可控制转变的纳米二氧化钛。一种方法是采用乙醇作溶剂的溶胶-凝胶法,通过控制SnCl₄的添加量,便可在450℃热处理下实现纳米TiO₂从纯锐钛矿到不同比例的复合相直至纯金红石相的转变。另一种方法是采用钛酸丁酯为原料直接低温水解,通过加入不同量的SnCl₄,制备了具有晶态结构的二氧化钛复合溶胶,在120℃下干燥处理便可实现TiO₂从锐钛矿到不同比例的复合相(金红石型、锐钛矿型和板钛矿型)直至纯金红石相的转变,制备所需晶态结构的纳米TiO₂。所有样品进行了透射电镜与XRD表征,制备的纳米TiO₂及其TiO₂-SnO₂纳米复合材料颗粒小、分布均匀、分散性好,没有检测到SnO₂晶体的X-衍射特征峰。     

Fe3O4纳米晶的简单调控合成、表征及磁性能

采用醋酸铵作保护剂在200℃下制备了单分散的400 nm粒径的Fe3O4空心纳米球.通过改变实验条件,对产品的形貌、内部结构和粒径进行了调控合成,得到了粒径范围在100～200 nm的实心纳米球和片形结构的Fe3O4纳米材料.采用SEM、TEM和XRD等对样品进行了表征.结果表明,所得尖晶石型Fe3O4纳米晶粒径均匀,分散度好.利用振动样品磁场计检测了不同形貌样品的磁性能.结果显示,Fe3O4纳米空心球的饱和磁化强度和矫顽力均大于Fe3O4纳米片的对应值.     

Fe2O3晶型对Fe基催化剂的CO2加氢性能影响

以共沉淀法制备FeAl母体,采用浸渍法添加Zn、K和Cu助剂制成催化剂,利用低温N2物理吸附、XRD、H2-TPR等手段对FeAl母体和催化剂进行表征,并用固定床反应器考察它们的CO₂加氢反应性能。XRD结果表明,加入Al助剂、并采用无水乙醇洗涤沉淀能促进酌-Fe₂O₃晶相生成,其中,Al₂O₃/Fe₂O₃质量比为10%的母体具有最强的酌-Fe₂O₃衍射峰;加入Al使得母体中的a-Fe₂O₃晶粒粒径变小,引起比表面积明显增大;浸渍助剂过程没有改变上述两种效应。母体比表面积增大提高了助剂Cu的分散度,促进了催化剂还原,但酌-Fe₂O₃晶相的生成才是催化剂的CO₂加氢反应活性被提高的主要原因。     

尼群地平晶型转变条件及其影响因素的确定

根据熔化数据推算相变稳定性理论计算了尼群地平不同晶型之间的相变温度, 并分别考察了高温、高温和高湿及高压条件下的晶型转变. 理论推导尼群地平I与II, 尼群地平I与III, 尼群地平II与III的转化温度分别为158.88, 160.50和158.65 ℃, 三者均为单变关系, 且在高温条件下尼群地平II, III都转变为尼群地平I, 在高压条件下, II易转变为I. 试验结果表明室温下尼群地平I为稳定型, II和III为亚稳定型, 3种晶型稳定性顺序为尼群地平I＞II＞III.     

P(St-co-MAA)乳液体系对CaCO3结晶的调控

大量研究表明, 有机/无机界面上的相互作用[1]是控制无机结晶的晶型、形貌、粒径等特征的决定因素. 本文利用乳液聚合方法合成了在诱导无机矿化后依然保持较为刚性界面的、能与无机离子作用的微球, 并在乳液中进行碳酸钙结晶实验, 用XRD, FTIR和SEM等手段对结晶进行了表征.     

GdPO4∶Eu3+和GdPO4∶Ce3+,Tb3+纳米晶多元醇法的合成与表征

首次采用多元醇的方法合成了GdPO4:Eu3+和GdPO4:Ce3+,Tb3+纳米晶,并利用X-射线衍射(XRD),傅立叶变换红外光谱(FTIR),透射电镜(TEM),光致发光光谱(PL)及热重和差示扫描量热分析(TG-DSC)对产物进行了表征.结果表明,产物为单斜晶系独居石结构正磷酸盐;形貌为梭形,长轴600～700 nm,短轴50～200 nm;纳米晶在水中有良好的分散性.GdPO4:Eu3+水溶液在251 nm激发下.发射光谱以Eu3+的5D0-7F1 (592 nm)磁偶极跃迁强度最大;GdPO4:Ce3+,Tb3+纳米晶水溶液的激发光谱在240～300nm处有一宽的吸收带,峰值位于262 nm,为Ce3+离子的4f-5d跃迁吸收,发射光谱呈现Tb3+特征绿色发射,最强峰位于544 nm.讨论了GdPO4:Ce3+,Tb3+体系中敏化发光机理,通过光谱分析证实了存在Ce3+→Gd3+→Tb3+的能量传递过程.     

Crystal structures of the novel hydrated borates Ba2B5O9(OH), Sr2B5O9(OH) and Li2Sr8B22O41(OH)2

Three novel hydrated borates Ba₂B₅O₉(OH) (1), Sr₂B₅O₉(OH) (2) and Li₂Sr₈B₂₂O₄₁(OH)₂ (3) have been synthesized hydrothermally and their structures determined. Compounds (1) and (2) are isostructural, crystallizing in space group P2₁/c and having lattice parameters of a=6.6330(13) Å, b=8.6250(17) Å, c=14.680(3) Å, β=93.46(3)° and a=6.4970(13) Å, b=8.4180(17) Å, c=14.177(3) Å, β=94.35(3)°, respectively. Compound (3) crystallizes in P-1 with lattice parameters of a=6.4684(13) Å, b=8.4513(17) Å, c=14.881(3) Å, α=101.21(3)°, β=93.96(3)°, γ=90.67(3)°. While similar in their axis lengths, (3) differs greatly in structure and formulation from (1) and (2). The structure of (1) and (2) is contrasted to that of the well-known mineral hilgardite (Ca₂B₅O₉Cl·H₂O).     

Syntheses and crystal structures of two new hydrated borates, Zn8[(BO3)3O2(OH)3] and Pb[B5O8(OH)]·1.5H2O

Two new hydrated borates, Zn₈[(BO₃)₃O₂(OH)₃] and Pb[B₅O₈(OH)]·1.5H₂O, have been prepared by hydrothermal reactions at 170 °C. Single-crystal X-ray structural analyses showed that Zn₈[(BO₃)₃O₂(OH)₃] crystallizes in a non-centrosymmetric space group R32 with a=8.006(2) Å, c=17.751(2) Å, Z=3 and Pb[B₅O₈(OH)]·1.5H₂O in a triclinic space group P1¯ with a=6.656(2) Å, b=6.714(2) Å, c=10.701(2) Å, α=99.07(2)°, β=93.67(2)°, γ=118.87(1)°, Z=2. Zn₈[(BO₃)₃O₂(OH)₃] represents a new structure type in which Zn-centered tetrahedra are connected via common vertices leading to helical ribbons _∞¹[Zn₈O₁₅(OH)₃]¹⁷⁻ that pack side by side and are further condensed through sharing oxygen atoms to form a three-dimensional _∞³[Zn₈O₁₁(OH)₃]⁹⁻ framework. The boron atoms are incorporated into the channels in the framework to complete the final structure. Pb[B₅O₈(OH)]·1.5H₂O is a layered compound containing double ring [B₅O₈(OH)]²⁻ building units that share exocyclic oxygen atoms to form a two-dimensional layer. Symmetry-center-related layers are stacked along the c-axis and held together by interlayer Pb²⁺ ions and water molecules via electrostatic and hydrogen bonding interactions. The IR spectra further confirmed the existence of both triangular BO₃ and OH groups in Zn₈[(BO₃)₃O₂(OH)₃], and BO₃, BO₄, OH groups as well as guest water molecules in Pb[B₅O₈(OH)]·1.5H₂O.     

Synthesis and ethylene polymerization behavior of {MeB(3-Ph-pyrazolyl)3}TiCl3

The new methyl-tris(pyrazolyl)borate reagents Li[MeTp^Ph] (1) [MeTp^Ph]⁻ = MeB(3-Ph-pyrazolyl)₃⁻) and Tl[MeTp^Ph] (2) react with TiCl₄ to afford (MeTp^Ph)TiCl₃ (3) in 77% and 81% yield respectively. 2 reacts with ZrCl₄ and HfCl₄ to yield mixtures of products. The reaction of 1 with TiCl₃(THF)₃ proceeds with B-N bond cleavage to afford TiCl₃(3-Ph-pyrazole)(THF)₂ as the major product (30%). The reaction of 3 with MeLi (3 equiv) yields 1 (60%) and reduced Ti species, via apparent displacement of [MeTp^Ph]⁻ and generation of unstable TiCl₄Me_4−x species. Under MAO activation conditions (MAO = methylalumoxane), 3 polymerizes ethylene to linear polyethylene. 3/MAO is significantly more active in ethylene polymerization than the hydrido-tris(pyrazolyl)borate analogue {HB(3-Ph-pyrazolyl)₃}TiCl₃/MAO.     

High-Pressure Synthesis and Crystal Structure of B2S3

Two new high-pressure phases of binary boron-sulfur compounds, B₂S₃-II and B₂S₃-III, were synthesized at 3-6.2 GPa. A single crystal of B₂S₃-III was grown and the structure was determined (tetragonal, space group I4₁/a, a=16.086(2) Å, c=30.488(4) Å; V=7888(1) ų, Z=100, R=3.0% and R_w=2.8% for 3047 observed data [I>3.00σ(I)]. The structure of B₂S₃-III consists of two kinds of macrotetrahedra built up from 20 and 34 BS₄-tetrahedra. These macrotetrahedra connect each other to form an interpenetrating zincblende-type structure by sharing BS₄-tetrahedra at the corners of those. B₂S₃-III is anticipated having a rather disordered structure. From the UV-Vis diffuse reflectance spectrum, the optical band gap of B₂S₃-III was estimated to be 3.7 eV.     

配合物[Ce(CH2=C(CH3)COO)2(NO3)(Bipy)]的合成及晶体结构

The new complex [Ce(CH₂=C(CH₃)COO)₂(NO₃)(Phen)]₂ was prepared in ethanol-aqueous solution with 8-hydroxyquinoline as the acidity regulator. Its crystal structure was determined by X-ray diffraction analysis. The title complex is triclinic, space group P1, a=1.00832(3)nm, b=1.02858(8)nm, c=1.12350(8)nm, α=113.9250(10)°, β=103.8210(10)°, γ=81.4650(10)°, V=1.03252(14)nm³, Z=1, D_c=1.700g·cm^-3, F(000)=522. The coordination number of Ce³⁺ is nine. CCDC: 211278.     

La3ScBi5的合成与晶体结构

在氩气保护下，将金属单质置于钽管中进行高温固相反应得到了一个新的三元极性金属间化合物,La₃ScBi₅。通过X-射线单晶衍射确定了它的晶体结构。La₃ScBi₅晶体属六方晶系，空间群为P6₃/mcm(No.193)，晶胞参数为：a=b=0.975 73(5) nm，c=0.655 92(6) nm，V=0.543 41(9) nm³，Z=2。La₃ScBi₅属反式Hf₅Sn₃Cu结构类型，其结构特征为Bi的一维直线链和由ScBi₆八面体之间通过共面形成的{ScBi₃}链。能带计算表明La₃ScBi₅呈金属导电性。     

在LiCl-KCl-AlCl3熔盐中直接电化学还原Sm2O3及Al-Sm合金的形成

在803 K LiCl-KCl熔盐中,研究了通过添加助剂AlCl3直接电化学还原Sm2O3和Al-Sm合金的形成。以SmCl3为原料作为参照,采用循环伏安和方波伏安方法,研究了Sm2O3在LiCl-KCl-AlCl3熔盐体系中的电化学行为。通过对比发现在两个体系中,峰的数量和位置基本一致,这说明在LiCl-KCl熔盐中,加入AlCl3之后,可以将Sm2O3有效氯化。计时电位结果表明,当阴极电流比-139.8 mA.cm-2更负时,Al和Sm共同还原。为了提取Sm,采用恒电流从LiCl-KCl-AlCl3-Sm2O3熔盐中电解得到Al-Sm合金样品,并进行XRD表征,结果表明可以通过调节AlCl3和Sm2O3的浓度得到不同相的Al-Sm合金。     

三苯基锡(Ⅳ)N-烃基哌嗪氨荒酸酯配合物的合成、表征、性质和Ph3SnS2CN(C2H4)2NCH3的晶体结构

Six triphenyltin(Ⅳ)N-alkylpiperazinyldithiocarbamates have been synthesized by the reaction of triphenyltin chloride with N-alkylpiperazinyldithiocarbamates and characterized by elemental analysis, UV, IR and ¹H NMR. The crystal structure of Ph₃SnS₂CN(C₂H₄)₂NCH₃(1) has been determined by X-ray single crystal diffraction. The crystal of the compound 1 belongs to triclinic with space group P1, a=1.033 56(18) nm, b=1.148 8(2) nm, c=1.191 6(2) nm, α=66.282(2)°, β=78.756(2)°, γ=67.476(2)°， Z=2, V=1.195 2(4) nm³, D_c=1.460 g·cm^-3, μ=1.256 mm^-1, R=0.025 1, wR=0.058 3. The structure shows a distorted tigonal bipyramidal configuration with five-coordination for the central tin atom. CCDC: 240375.     

在LiCl-KCl-AlCl3熔盐中直接电化学还原Sm2O3及Al-Sm合金的形成

在803 K LiCl-KCl熔盐中, 研究了通过添加助剂AlCl₃直接电化学还原Sm₂O₃和Al-Sm合金的形成。以SmCl₃为原料作为参照, 采用循环伏安和方波伏安方法, 研究了Sm₂O₃在LiCl-KCl-AlCl₃熔盐体系中的电化学行为。通过对比发现在两个体系中, 峰的数量和位置基本一致, 这说明在LiCl-KCl熔盐中, 加入AlCl₃之后, 可以将Sm₂O₃有效氯化。计时电位结果表明, 当阴极电流比-139.8 mA·cm^-2更负时, Al和Sm共同还原。为了提取Sm, 采用恒电流从LiCl-KCl-AlCl₃-Sm₂O₃熔盐中电解得到Al-Sm合金样品, 并进行XRD表征, 结果表明可以通过调节AlCl₃和Sm₂O₃的浓度得到不同相的Al-Sm合金。