Pt/K2La2Ti3O10催化剂的合成及其光催化分解甲醇水溶液制氢

用高温固相法合成了具有类钙钛矿型结构的层状化合物K₂La₂Ti₃O₁₀, 用XRD, UV-DRS对其进行表征. 利用不同还原方法制备了Pt/K₂La₂Ti₃O₁₀光催化剂, 并且用脉冲氢氧滴定法(HOT)测定了K₂La₂Ti₃O₁₀表面Pt的分散度. 考察了Pt/K₂La₂Ti₃O₁₀光催化分解甲醇水溶液制氢的活性. 比较了负载Pt与负载Ni和纯的K₂La₂Ti₃O₁₀的光催化活性. 研究了Pt负载量、不同还原方法对光催化分解水制氢反应活性的影响. 在最佳的Pt负载量2%(质量百分比)下, 产氢速率达到233.88 mmol·h^&;#8722;1. 讨论了该催化剂的能带结构及反应机理.     

Cr掺杂对K2La2Ti3O10光催化活性的影响

通过溶胶-凝胶法制备了层状钙钛矿结构的K₂La₂Ti₃O₁₀及Cr掺杂的K₂La₂Ti₃O₁₀，采用X-射线衍射(XRD)、紫外可见漫反射光谱(DRS)、X射线光电子能谱(XPS)等对K₂La₂Ti₃O₁₀及Cr掺杂K₂La₂Ti₃O₁₀进行了表征。以I^-为电子给体、分别在紫外和可见光辐射下研究了K₂La₂Ti₃O₁₀及Cr掺杂K₂La₂Ti₃O₁₀光催化分解水的产氢活性。采用第一性原理，计算了Cr掺杂对K₂La₂Ti₃O₁₀半导体能带结构和态密度的影响，从电子结构的变化揭示了掺杂引起光催化活性差异的原因。结果表明，Cr的掺入能够改善和提高K₂La₂Ti₃O₁₀的光解水的产氢活性；Cr改善和提高K₂La₂Ti₃O₁₀的光解水的产氢活性存在一个最佳的掺杂浓度；当Cr与Ti的物质量的比为0.02∶1时，紫外光催化分解水产氢速率为1 500 μmol·L^-1·h^-1，可见光催化分解水产氢速率为83.6 μmol·L^-1·h^-1，分别为K₂La₂Ti₃O₁₀掺杂改性前产氢速率的26和5倍。     

固体电解质La2-xCaxMo1.7W0.3O9-δ(0≤x≤0.2)的合成、表征及电性能

在氧离子导体La₂Mo_1.7W_0.3O₉的基础上，采用固相法合成了La位掺杂的Ca系列新型氧化物La_2-xCa_xMo_1.7W_0.3O_9-δ(0≤x≤0.2)。通过XRD、Raman和XPS等手段对化合物结构进行表征，交流阻抗谱测试其电性能。结果表明：掺杂离子Ca²⁺的半径小于基质离子La³⁺的半径导致晶格收缩；Ca的掺杂在La₂Mo_1.7W_0.3O₉自身内置氧空位的基础上增加了额外的氧空位，提高了氧离子导体的电导率，550 ℃电导率由0.79 × 10^-4 S·cm^-1 (x=0.0)增加到1.5 × 10^-4 S·cm^-1 (x=0.16，0.2)，电导率增加89.9%。     

电荷补偿对Ba2ZnGe2O7∶Bi3+荧光粉发光性质的影响

采用高温固相法制备了2个系列的荧光粉样品：Ba_2-xZnGe₂O₇∶xBi³⁺(系列Ⅰ)和Ba_1.994-yK_yZnGe₂O₇∶0.006Bi³⁺(系列Ⅱ)。X射线衍射(XRD)测试结果表明,少量Bi³⁺、K⁺的掺杂不会明显改变材料的物相结构。样品的荧光光谱测试结果表明,虽然2个系列样品的发光光谱都随组成成分变化有少量变化,但发光颜色基本上均为黄绿色。在358 nm的激发下,荧光粉的发射光谱呈现一个峰值在 500 nm 的宽发射带,归属于 ³P₁→^1S₀能级跃迁。在 500 nm 监测下,荧光粉的最强激发峰位于 358 nm,归属于¹S₀→³P₁能级跃迁,此外还有一个位于320 nm的肩峰归属于O^2--Bi³⁺电荷转移带。系列Ⅰ样品的光谱数据结果指出,Bi³⁺的最佳掺杂量x为0.006。在该基质中,Bi³⁺掺杂取代Ba²⁺属于不等价取代,会在晶格中产生Ba²⁺空位或间隙O^2-,对材料的发光强度产生负面影响。对此,采用K⁺与Bi³⁺协同掺杂起到电荷补偿的作用,填补Ba²⁺空位或捕获间隙O^2-缺陷。空位被填补或间隙被捕获均减少了晶格畸变,从而使发光强度明显提高。系列Ⅱ样品的光谱数据表明,完全电荷补偿的荧光粉样品相比于没有掺K⁺的样品,其发光强度提高了约2.5倍。     

电荷补偿对Ba2ZnGe2O7：Bi3+荧光粉发光性质的影响

采用高温固相法制备了2个系列的荧光粉样品：Ba_2-xZnGe₂O₇：xBi³⁺（系列Ⅰ）和Ba_1.994-yK_yZnGe₂O₇：0.006Bi³⁺（系列Ⅱ）。X射线衍射（XRD）测试结果表明,少量Bi³⁺、K⁺的掺杂不会明显改变材料的物相结构。样品的荧光光谱测试结果表明,虽然2个系列样品的发光光谱都随组成成分变化有少量变化,但发光颜色基本上均为黄绿色。在358 nm的激发下,荧光粉的发射光谱呈现一个峰值在500 nm的宽发射带,归属于³P₁→¹S₀能级跃迁。在500 nm监测下,荧光粉的最强激发峰位于358 nm,归属于¹S₀→³P₁能级跃迁,此外还有一个位于320 nm的肩峰归属于O^2--Bi³⁺电荷转移带。系列Ⅰ样品的光谱数据结果指出,Bi³⁺的最佳掺杂量x为0.006。在该基质中,Bi³⁺掺杂取代Ba²⁺属于不等价取代,会在晶格中产生Ba²⁺空位或间隙O^2-,对材料的发光强度产生负面影响。对此,采用K⁺与Bi³⁺协同掺杂起到电荷补偿的作用,填补Ba²⁺空位或捕获间隙O^2-缺陷。空位被填补或间隙被捕获均减少了晶格畸变,从而使发光强度明显提高。系列Ⅱ样品的光谱数据表明,完全电荷补偿的荧光粉样品相比于没有掺K⁺的样品,其发光强度提高了约2.5倍。     

Li3V2(PO4)3电极过程及其锂离子脱嵌动力学研究(I)

采用溶胶凝胶法合成了Nasicon化合物Li₃V₂(PO₄)₃, 采用X射线衍射(XRD)对产品进行了物相分析. 采用充放电测试, 循环伏安(CV)研究了化合物的电化学性能和锂离子的脱嵌过程, 计算出Li^＋在固相中的扩散系数(10^－8 cm²•s^－1); 采用交流阻抗测试(EIS)研究了Li₃V₂(PO₄)₃的电极过程; 对两种类型的阻抗图谱提出不同等效电路模型并对结果进行了拟合; 研究了Li₃V₂(PO₄)₃电极过程动力学以及新鲜电极界面在充放电过程中的变化特性.     

Li3V2(PO4)3电极过程及其锂离子脱嵌动力学研究(I)

采用溶胶凝胶法合成了Nasicon化合物Li₃V₂(PO₄)₃, 采用X射线衍射(XRD)对产品进行了物相分析. 采用充放电测试, 循环伏安(CV)研究了化合物的电化学性能和锂离子的脱嵌过程, 计算出Li^＋在固相中的扩散系数(10^－8 cm²•s^－1); 采用交流阻抗测试(EIS)研究了Li₃V₂(PO₄)₃的电极过程; 对两种类型的阻抗图谱提出不同等效电路模型并对结果进行了拟合; 研究了Li₃V₂(PO₄)₃电极过程动力学以及新鲜电极界面在充放电过程中的变化特性.     

Ca9Y(PO4)7:Ce3+,Tb3+纳米荧光粉的制备及发光性能

采用水热法制备出Ca₉Y（PO₄）₇：Ce³⁺,Tb³⁺纳米荧光粉,通过XRD、SEM和荧光光谱等对样品进行了分析,研究在Ca₉Y（PO₄）₇基质中引入Ce³⁺,Tb³⁺离子对发光性能的影响规律。研究发现因Tb³⁺离子自身能量交叉驰豫的存在,使得单掺Tb³⁺时,通过调节Tb³⁺离子的浓度可以实现对发光颜色的控制。同时研究了Ce³⁺-Tb³⁺之间的能量传递为电多极相互作用的偶极-四极机制,Ce³⁺-Tb³⁺之间最大的能量传递效率为55.6%。Ca₉Y（PO₄）₇：Ce³⁺,Tb³⁺的发光颜色可以通过激活离子之间的能量传递和共发射得到可控调节。SEM分析表明荧光粉颗粒尺寸在100 nm左右,分散性好。     

298.15 K Li2B4O7-MgCl2-H2O体系热力学性质的电动势法测定及离子相互作用模型的研究

测定了298.15 K下, 无液接电池Li-ISE│Li₂B₄O₇ (m_A)(aq.), MgCl₂(m_B)(aq.)│AgCl/Ag的电动势, 利用测定结果计算了Li₂B₄O₇-MgCl₂-H₂O体系离子强度在0.05～3 mol•kg^－1范围内, 不同MgCl₂离子强度分数的溶液中LiCl的平均活度系数, 并给出了其随离子强度I, B₄O₇^2－和Mg^2＋浓度的变化规律. 结合以往关于该体系和Li₂B₄O₇-LiCl-H₂O, Li₂B₄O₇-H₂O体系的等压研究结果, 用迭代和多元线性回归方法对Li^＋-Mg^2＋-Cl^－-B₄O₇^2－-H₂O体系的离子相互作用模型进行了研究. 具体方法为考虑了该体系在不同的总硼浓度范围H₃BO₃, B(OH)₄^－, B₃O₃(OH)₄^－和B₄O₅(OH)₄^2－四种含硼化合物的存在以及各硼化合物间的化学平衡, 以修正了的Pitzer渗透系数方程和活度系数方程为基础, 对该体系的等压法和电动势法研究结果进行最小二乘拟合, 拟合的标准偏差为0.0167, 用该模型计算的该体系的渗透系数、活度系数与实验值基本一致.     

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.     

Phase stability and ionic conductivity in substituted La2W2O9

Different substitutions, i.e. Sr²⁺, Ba²⁺, K⁺, Nb⁵⁺ and V⁵⁺, have been performed in the triclinic α-La₂W₂O₉ structure in order to stabilise the high temperature and better ionic conductor cubic β-phase. This approach has been used to try to obtain a new series of ionic conductors with LAMOX-type structure without molybdenum and presumably better redox stability compared to β-La₂Mo₂O₉. Nanocrystalline materials obtained by a freeze-drying precursor method at 600 °C exhibit mainly the β-La₂W₂O₉ structure, however, the triclinic α-form is stabilised as the firing temperature increases and the crystallite size grows. Only high levels of Ba²⁺ and V⁵⁺ substitutions retained the cubic form at room temperature after firing above 1100 °C. However, these phases are metastable above 700 °C, exhibiting an irreversible transformation to the low temperature triclinic α-phase. The synthesis, structure, phase stability, kinetic of phase transformation and electrical conductivity of these materials have been studied in the present report.     

Electronic polarizability and crystallization of K2O-TiO2-GeO2 glasses with high TiO2 contents

Some K₂O-TiO₂-GeO₂ glasses with a large amount of TiO₂ contents (15-25 mol%) such as 25K₂O-25TiO₂-50GeO₂ have been prepared, and their electronic polarizability, Raman scattering spectra, and crystallization behavior are examined to clarify thermal properties and structure of the glasses and to develop new nonlinear optical crystallized glasses. It is proposed that the glasses consist of the network of TiO₆ and GeO₄ polyhedra. The glasses show large optical basicities of Λ=0.88-0.92, indicating the high polarizabity of TiO_n (n=4-6) polyhedra in the glasses. K₂TiGe₃O₉ crystals are formed through crystallization in all glasses prepared in the present study. In particular, 20K₂O-20TiO₂-60GeO₂ glass shows bulk crystallization and 18K₂O-18TiO₂-64GeO₂ glass exhibits surface crystallization giving the c-axis orientation. The crystallized glasses show second harmonic generations (SHGs), and it is suggested that the distortion of TiO₆ octahedra in K₂TiGe₃O₉ crystals induces SHGs.     

Base-promoted reaction of C60Cl6 with thioamides: an access to [60]fullereno[1,9-d] thiazoles

Regioselective reaction of C₆₀Cl₆ with thioamides via a radical annulation to form fullereno thiazole derivatives is reported. The reaction is promoted by K₂CO₃, which might deprotonate thioamide to initiate a single electron transfer from thioamide anion to C₆₀Cl₆. The experiments with various thioamides establish the proposed base-promoted reaction as a facile route for synthesis of fullereno fused thiazole derivatives starting from C₆₀Cl₆, a prevalent synthon in fullerene chemistry. In addition, the tunable electrochemical properties of the fullereno thiazole products have been investigated for their potential photovoltaic application.     

Non-centrosymmetric Ba3Ti3O6(BO3)2

The compound previously reported as Ba₂Ti₂B₂O₉ has been reformulated as Ba₃Ti₃B₂O₁₂, or Ba₃Ti₃O₆(BO₃)₂, a new barium titanium oxoborate. Small single crystals have been recovered from a melt with a composition of BaTiO₃:BaTiB₂O₆ (molar ratio) cooled between 1100°C and 850°C. The crystal structure has been determined by X-ray diffraction: hexagonal system, non-centrosymmetric space group, a=8.7377(11) Å, c=3.9147(8) Å, Z=1, wR(F²)=0.039 for 504 unique reflections. Ba₃Ti₃O₆(BO₃)₂ is isostructural with K₃Ta₃O₆(BO₃)₂. Preliminary measurements of nonlinear optical properties on microcrystalline samples show that the second harmonic generation efficiency of Ba₃Ti₃O₆(BO₃)₂ is equal to 95% of that of LiNbO₃.     

PbS插层K2Ti4O9催化剂：制备及光催化制氢活性

利用高温固相反应、离子交换、层间插入反应和硫化处理制备了PbS插层的K2Ti4O9催化剂。利用XRD、TEM、SEM、XRF、PL和紫外-可见漫反射光谱对催化剂进行了表征,考察了催化剂紫外光和可见光光催化制氢活性。结果表明,制备的PbS插层K2Ti4O9催化剂对可见光的吸收范围较宽,其吸收边界约为710 nm,在紫外光和可见光下3 h累积产氢量可达到115.46 mmol.gcat-1和0.92 mmol.gcat-1,与CdS插层K2Ti4O9催化剂相比具有更高的催化活性。     

Zr1−xLnxW2O8−x/2 (Ln=Eu, Er, Yb): Solid solutions of negative thermal expansion-synthesis, characterization and limited solid solubility

Zr_1−xLn_xW₂O_8−x/2 solid solutions (Ln=Eu, Er, Yb) of different substitution fractions x have been synthesized. Their X-ray diffraction (XRD) patterns have been indexed and lattice parameters calculated based on the α-ZrW₂O₈ structure. The coefficients of thermal expansion (CTEs) of these solid solutions were estimated to be −10.3×10⁻⁶ K⁻¹ in temperature range of 30-100 °C. The solubility of lanthanide ions in these solid solutions decreases linearly with the increase in the radius of substituted lanthanide ions. Based on the concentration dependence of phase transition temperatures, a novel method for determination of solubility of the lanthanide ions in Zr_1−xLn_xW₂O_8−x/2 solid solutions has been developed. This method seems to be more sensitive as compared with that based on XRD technique.     

Ce掺杂K2La2Ti3O10催化剂的可见光高效催化制氢的研究

采用高温固相法合成了铈掺杂的K₂La₂Ti₃O₁₀催化剂, 利用X射线衍射(XRD)、紫外-可见漫反射(UV-vis DRS)、透射电镜(TEM)和X射线光电子能谱(XPS)对催化剂进行了表征. 考察了催化剂的可见光催化分解甲醇水溶液制氢的活性, 并对可见光催化机理进行了分析. 研究表明, 铈的掺杂没有改变K₂La₂Ti₃O₁₀的微晶结构, 并使催化剂粒径有所减小. 紫外可见漫反射分析表明禁带宽度为2.3 eV左右, 对可见光具有较高吸收. XPS表明La和Ti为＋3和＋4价, 而Ce则是＋3和＋4的混合价态. 担载2 wt% Pt后, 在可见光下光催化活性大大提高, 当铈的掺杂量为0.5 mol%(即Ce取代La的摩尔百分量)时, 光催化活性达到最大, 产氢速率为0.05 mmol/h; 光照5 h后产氢量为0.22 mmol, 而纯K₂La₂Ti₃O₁₀的产氢量只有0.037 mmol.     

Determination of dissociation degrees of K3NbF8 and K3TaF8 by thermodynamic analysis of subsystems of the KF-K2NbF7 and KF-K2TaF7 systems

A special form of the LeChatelier-Shreder equation describing the equilibrium between the crystalline phase and the melt in system A-AB in which the substance AB partially dissociates upon melting was applied to systems KF-K₃NbF₈, K₂NbF₇-K₃NbF₈ and to KF-K₃TaF₈, K₂TaF₇-K₃TaF₈ subsystems of the binary systems KF-K₂NbF₇ and KF-K₂TaF₇ in which the additive compounds K₃NbF₈ and K₃TaF₈ are formed. Using the phase diagram of the system KF-K₂NbF₇ determined by McCawley and Barclay (1971) and the values of the fusion enthalpy of K₃NbF₈ taken from literature, the intervals of the dissociation degree values of K₃NbF₈ for both branches of the liquidus curve of K₃NbF₈ were calculated. The calculated values of the dissociation degree depend on the coordinates of the liquidus curve of K₃NbF₈ of the pertinent phase diagram, on its used branch and section, and on the value of the fusion enthalpy of K₃NbF₈. For the measured fusion enthalpy of K₃NbF₈ (57 kJ mol⁻¹), a common interval of the dissociation degree values of K₃NbF₈ for both branches of the liquidus curve of K₃NbF₈ is 0.71–0.72. Similarly, intervals of the dissociation degree values of K₃TaF₈ for both branches of the liquidus curve of K₃TaF₈ were calculated using the phase diagram of the system KF-K₂TaF₇ determined by Boča et al. (2007) and the measured fusion enthalpy of K₃TaF₈ ((52 ± 2) kJ mol⁻¹). The error of the determination of the fusion enthalpy of K₃TaF₈, the common interval of the dissociation degree values of K₃TaF₈ for both branches of the liquidus curve of K₃TaF₈ is 0.68–0.69.     

Influence of Pd precursors on the catalytic performance of Pd–H4SiW12O40/SiO2 in the direct oxidation of ethylene to acetic acid

The effects of palladium precursors (PdCl₂, (NH₄)₂PdCl₄, Pd(NH₃)₂Cl₂, Pd(NO₃)₂ and Pd(CH₃COO)₂) on the catalytic properties in the selective oxidation of ethylene to acetic acid have been investigated for 1.0 wt% Pd–30 wt% H₄SiW₁₂O₄₀/SiO₂. The structures of the catalysts were characterized using X-ray diffraction, N₂ adsorption, H₂-pulse chemical adsorption, infrared spectrometry of the adsorbed pyridine, H₂ temperature-programmed reduction and X-ray photoelectron spectroscopy. The present study demonstrates that the different palladium precursors can lead to the significant changes in the dispersion of palladium. It is found that Pd dispersion decreases as follows: PdCl₂ > (NH₄)₂PdCl₄ > Pd(NO₃)₂ > Pd(NH₃)₂Cl₂ > Pd(C₂H₃O₂)₂, which is nearly identical to the catalytic activity. This indicates that the dispersion of palladium plays an important role in the catalytic activity. Furthermore, density of Lewis (L) and Brönsted (B) acid sites are also strongly dependent on the palladium precursors. It is also demonstrated that an effective catalyst should possess a well combination of Brönsted acid sites with dispersion of palladium.