Sn4+-TiO2的制备及其光催化降解苯酚的研究

采用硬脂酸法制备出Sn4+-TiO2复合光催化剂,用透射电子显微镜和X射线衍射仪对粉体的粒径、物相、形貌和热稳定性进行了表征.通过粉体对苯酚的降解情况对其光催化活性进行了测试,结果表明,与纯TiO2相比,Sn4+-TiO2的光催化活性有较大提高,当SnO2的掺入量为摩尔比5.0%时催化活性最高.     

Sn~(4+)-TiO_2的制备及其光催化降解苯酚的研究

采用硬脂酸法制备出Sn4+-TiO2复合光催化剂,用透射电子显微镜和X光衍射仪对粉体的粒径、物相、形貌和热稳定性进行了表征。样品经500℃焙烧2h后,5%Sn4+-TiO2纳米粉末颗粒细小均匀,形状完整,粉末的平均晶粒度约为14nm。通过粉体对苯酚的降解情况对其光催化活性进行了测试,结果表明,与纯TiO2相比,Sn4+-TiO2的光催化活性有较大提高,当SnO2的掺入量为摩尔比5.0%时催化活性最高。以高压汞灯为光源,苯酚的初始浓度为80mg.L-1、催化剂5%Sn4+-TiO2投加量为1.0g.L-1时,溶液的pH为4,苯酚的光催化降解效果最好。     

SnP2+-TiO2的可见光催化活性及其在介孔蒙脱石上的负载

分别以氯化锡和氯化亚锡为Sn源,使用溶胶-凝胶法制备出不同掺杂量的Sn-TiO2,比较了Sn2+与Sn4+对掺杂后TiO2可见光催化活性的影响.实验结果显示,Sn2+与Sn4+均能显著抑制TiO2晶粒生长,并促进其晶型转变.但Sn2+-TiO2的可见光催化活性却明显优于Sn4+-TiO2,这主要是Sn2+外层半充满的电子轨道结构引起的.将可见光催化活性很高的Sn2+-TiO2负载于大比表面积、高稳定性的介孔蒙脱石上,由于载体与Sn-TiO2之间发生了相互作用,负载后样品的UV-Vis光谱吸收边相对于Sn-TiO2发生了显著红移,且可见光催化活性也有大幅提高.     

Sm3+和Gd3+共掺杂TiO2粉体的制备和性能表征

采用溶胶-凝胶法制备了纯TiO2,1%Sm3+或2%Gd3+单掺杂和1%Sm3+/2%Gd3+共掺杂TiO2复合粉体,采用XRD和SEM/EDAX等技术进行表征。以对亚甲基蓝的光催化降解为目标反应,评价了TiO2复合粉体的光催化活性,探讨了Sm3+/Gd3+共掺杂、亚甲基蓝初始浓度和粉体投加量对TiO2粉体光催化活性的影响机制。结果表明,Sm3+/Gd3+共掺杂可以显著提高TiO2粉体的光催化活性;Sm3+/Gd3+共掺杂在TiO2粉体中产生协同作用,抑制了TiO2由锐钛矿相向金红石相转变,使TiO2粒径尺寸减小,增大了TiO2的晶格畸变。当亚甲基蓝初始浓度为4mg/L和粉体投加量为2g/L时,TiO2复合粉体的光催化活性最高,对亚甲基蓝光催化降解率达99.71%;降解亚甲基蓝反应符合Langmuir-Hinshelwood动力学方程。     

金属离子掺杂TiO2的光催化性能研究

用醇盐水解法制备了Ce4+、Ag+、Fe3+、Fe2+、Sn4+、Zn2+、Mo6+等金属离子掺杂的TiO2复合微粒.以罗丹明6G降解为目标反应,研究了所制备的复合微粒光催化活性与选择性.并用IR、XRD、TEM及BET等技术,对TiO2复合微粒进行了表征.结果显示在TiO2内掺入Ce4+、Ag+、Sn4+,可使纳米TiO2的光催化活性增强,而Fe3+、Fe2+、Zn2+、Mo6+等金属离子掺杂的二氧化钛复合微粒的催化活性呈下降趋势.     

尖晶石型铁氧体CaxZn1-xFe2O4的制备及其光催化性能研究

采用改进的溶胶-凝胶法制备CaxZn1-xFe2O4粉体。用X射线粉末衍射仪(XRD)对样品进行结构表征,随着Ca2+掺杂量的增加,样品出现CaFe2O4的衍射峰。使用扫描电子显微镜(SEM)对样品进行形貌表征,结果表明样品的形貌呈不规则的颗粒状,且颗粒大小为2μm,并显现出片层堆叠情况。通过对甲基橙进行光催化降解实验,对CaxZn1-xFe2O4粉体的光催化活性进行了研究。结果表明,经过Ca2+掺杂的CaxZn1-xFe2O4样品,光催化活性明显提高。     

Fe对Mn/CeO2-TiO2催化剂低温NH3选择性催化还原NO的影响

以锰氧化物为活性组分,CeO2-TiO2为载体制备了Mn/CeO2-TiO2催化剂.考察了Fe的加入对Mn/CeO2-TiO2的低温NH3-SCR活性的影响.并采用BET比表面积,H2程序升温还原(H2-TPR)和X射线光电子能谱(XPS)等手段对催化剂进行了表征.活性结果表明,Fe的引入显著改善了Mn/CeO2-TiO2的NH3-SCR活性,催化剂在113～250℃之间表现出良好的NO去除效率.表征结果表明,Fe的引入促进了锰物种在CeO2-TiO2表面的分散,降低了Mn-Fe/CeO2-TiO2中锰物种的还原温度.XPS分析指出Mn-Fe/CeO2-TiO2表面Mn以+4价存在,而Fe主要以+3价的Fe2O3存在,且Fe与载体表面间存在强相互作用.     

磁性La3+掺杂TiO2的制备及性能

利用溶胶-凝胶法,在室温条件下,以钛酸四丁酯、硝酸镧为主要原料,无水乙醇为溶剂,冰醋酸为抑制剂,浓硝酸为催化剂制得稳定的掺La3+TiO2溶胶,陈化后的凝胶经不同温度煅烧3h后制得不同掺La3+量的TiO2。通过XRD对不同煅烧温度及不同掺La3+量的TiO2进行了表征;以紫外光为光源,研究了掺La3+-TiO2对甲基橙溶液的光降解效果。用化学共沉淀法制备了具有强磁性的Fe3O4水基磁流体,再与La3+掺杂TiO2进行复合,制备了Fe3O4负载量不同的磁性La3+掺杂TiO2,研究了Fe3O4负载量不同的La3+掺杂TiO2对甲基橙的光催化降解效果、磁分离回收率的影响。结果表明,掺La3+量及煅烧温度对TiO2的晶型、各晶型TiO2的相对含量及对甲基橙的光降解效果均有影响。La3+掺杂TiO2比纯TiO2显示出更强的光催化性能,掺La3+量2%,热处理温度450℃的La3+掺杂TiO2光催化活性最高。Fe3O4负载量为10%的Fe3O4/La3+-TiO2对甲基橙的降解率8h时为99.4%;磁分离回收率达97.39%。     

Fe_3O_4/Ce~(3+)-TiO_2复合光催化材料的制备及其光催化性能研究

采用溶胶-凝胶法,以钛酸四丁酯、硝酸铈为主要原料,无水乙醇为溶剂,冰醋酸为抑制剂,浓硝酸为催化剂制得稳定的Ce3+掺杂TiO2溶胶,其凝胶经不同温度煅烧3 h后制得Ce3+掺杂量不同的TiO2粉体。用XRD对TiO2进行了测试对比分析,以紫外光为光源,亚甲基蓝溶液为模拟有机染料废水,研究了TiO2的光催化性能。用化学共沉淀法制备了具有强磁性的纳米Fe3O4水基磁流体,再与Ce3+掺杂TiO2进行复合,制备了Fe3O4负载量不同的磁性Ce3+掺杂TiO2,研究了其对亚甲基蓝的光催化降解效果、磁分离回收率的影响。结果表明,TiO2凝胶热处理温度、Ce3+掺量、TiO2晶型及Fe3O4负载量对亚甲基蓝的光催化活性均有影响。掺Ce3+量为1%,热处理温度650℃的Ce3+掺杂TiO2粉体光催化活性最高。Fe3O4负载量为10%的Fe3O4/Ce3+-TiO2对亚甲基蓝的降解率8 h时达到90.3%,磁分离回收率达96.8%。     

环境净化功能TiO2/SiO2复合纳米粉体的制备与表征

以锐钛矿型TiO2纳米粉体为载体,Na2SiO3为包覆剂,H2SO4为中和剂,采用溶胶-凝胶法制备了系列环境净化功能TiO2/SiO2复合纳米粉体.用XRD、XRF、TEM、BET比表面分析对其进行了表征,并以亚甲基蓝溶液的光催化降解率和COD去除率为指标评价了其光催化活性.结果表明,在TiO2纳米颗粒表面包覆一层多孔非晶态水合二氧化硅纳米膜,可以显著提高其水分散性,有效控制其光催化活性,进而提高了涂料的抗老化性和耐候性.中和时间对包硅效率影响较大,适当增加中和时间有利于提高包硅效率;包覆温度对包硅效率影响较小,升高温度使包硅效率略有降低.低温包覆,成膜相对疏松,改性粉体的光催化活性相对较高;高温包覆,成膜相对致密,改性粉体的光催化活性相对较低.     

Varistor properties of ZnO-Pr6O11-CoO-Cr2O3-Y2O3-In2O3 ceramics

The varistor properties of the ZnO-Pr₆O₁₁-CoO-Cr₂O₃-Y₂O₃-In₂O₃ ceramics were investigated for different concentrations of In₂O₃. The increase of In₂O₃ concentration slightly increased the sintered density (5.60-5.63 g/cm³) and slightly decreased the average grain size (3.4-2.9 μm). The breakdown field increased from 6023 to 14822 V/cm with increasing concentration of In₂O₃. The nonlinear coefficient increased from 17.6 to 44.6 for up to 0.005 mol%, whereas the further doping caused it to decrease to 36.8. In₂O₃ acted as an acceptor due to the donor concentration, which decreases in the range of 1.02 × 10¹⁷ to 0.24 × 10¹⁷/cm³ with increasing concentration of In₂O₃.     

Nanocrystallization of SrBi2Nb2O9 from glasses in the system Li2B4O7---SrO---Bi2O3---Nb2O5

Transparent glasses in the system (100−x)Li₂B₄O₇–x(SrO---Bi₂O₃---Nb₂O₅) (10≤x≤60) (in molar ratio) were fabricated by a conventional melt-quenching technique. Amorphous and glassy characteristics of the as-quenched samples were established via X-ray powder diffraction (XRD) and differential thermal analyses (DTA) respectively. Glass–ceramics embedded with strontium bismuth niobate, SrBi₂Nb₂O₉ (SBN) nanocrystals were produced by heat-treating the as-quenched glasses at temperatures higher than 500 °C. Perovskite SBN phase formation through an intermediate fluorite phase in the glass matrix was confirmed by XRD and transmission electron microscopy (TEM). Infrared and Raman spectroscopic studies corroborate the observation of fluorite phase formation. The dielectric constant (_r) and the loss factor (D) for the lithium borate, Li₂B₄O₇ (LBO) glass comprising randomly oriented SBN nanocrystals were determined and compared with those predicted based on the various dielectric mixture rule formalism. The dielectric constant was found to increase with increasing SBN content in LBO glass matrix.     

Syntheses of hollandite type Rb2Cr8O16, K2Cr2V6O16 and K2V8O16

Hollandite-type compounds, Rb₂Cr₈O₁₆, K₂Cr₂V₆O₁₆ and K₂V₈O₁₆, were synthesized under high P-T conditions up to 1200°C and 7GPa. The structural refinement using a single crystal of Rb₂Cr₈O₁₆ confirms that the structure is similar to that of K₂Cr₈O₁₆. Magnetic measurements indicate that Rb₂Cr₈O₁₆ is ferromagnetic below 295K, K₂Cr₂V₆O₁₆ paramagnetic down to 77K and K₂V₈O₁₆ has susceptibility anomaly at 175K. These compounds are all semiconductive and show discontinuities in temperature-resistivity curves at points corresponding to magnetic anomalies.     

Characterization of YBa2Cu3O7/PrBa2Cu3O7 superlattices

We investigated the structural and superconducting properties ofc-axis oriented (YBa₂Cu₃O₇) _nY /(PrBa₂Cu₃O₇) _npr superlattices with thicknesses of the individual layers down to one unit cell (10nY1; 18>nPr 1). By transmission electron microscopy and X-ray diffraction we find an excellent structural quality of the samples, though the quantitative analysis shows the existence of defects. In superlattices with decoupled YBa₂Cu₃O₇ layers of two unit cell thickness we find a highT _c value of 75 K. We probed the flux line structure in the superlattices by measurements of the critical current density in magnetic fields. The experiments show that the flux-line dynamics is dominated by the movement of pancake vortices.     

Magnetic coupling in La0.67Ca0.33MnO3/La0.67Sr0.33CoO3/La0.67Ca0.33MnO3 sandwiches

La_0.67Ca_0.33MnO₃ (LCMO)/La_0.67Sr_0.33CoO₃ (LSCO)/LCMO trilayer films are fabricated on single-crystal substrates NdGaO₃ (110) and the interlayer coupling are investigated. Compared with LCMO single layer, sandwiches showed the enhanced metal-insulator transition temperature of LCMO layers. The magnetoresistance is dependent on spacer thickness and the peak value dramatically decreases when LSCO layer is thick enough because of shorting by the LSCO layer. The magnetic coercivity H_C shows a nonmonotonic behavior with changing spacer layer thickness and the waist-like hysteresis indicates that there is an indirect exchange coupling between the top and bottom LCMO layers across the spacer layer.     

The effect of Bi1.5Zn0.5Nb0.5Ti1.5O7 cover layer on the dielectric and tunable properties of Ba0.6Sr0.4TiO3/Bi1.5Zn0.5Nb0.5Ti1.5O7 bilayered thin films

Bi_1.5Zn_0.5Nb_0.5Ti_1.5O₇ (BZNT) thin films with different thicknesses as cover layers were deposited on the Ba_0.6Sr_0.4TiO₃ (BST) thin films on the Pt/Ti/SiO₂/Si substrates by radio frequency magnetron sputtering method. The microstructure, surface morphology, dielectric and tunable properties of BST/BZNT heterogeneous bilayered films were investigated as a function of the thickness of BZNT films and the effect of BZNT films on the asymmetric electrical properties of BST/BZNT bilayered films was discussed. It was found that BZNT cover layer significantly improved the leakage current and the dielectric loss, and the dielectric constant and tunability of BST/BZNT bilayered thin films simultaneously decreased with the increasing thickness of BZNT films. The BST/BZNT bilayered thin film with a 50 nm BZNT cover layer gave the largest figure of merit (FOM) of 33.48 with the upper tunability of 55.38%. The asymmetric electrical behavior of BST/BZNT bilayered films is probably related to an internal electric field caused by built-in voltages at Pt/BST and BZNT/Au interfaces.     

Microstructures of YBa2Cu3O7/La0.7Ca0.3MnO3 and La0.7Ca0.3MnO3/YBa2Cu3O7 bi-layers grown on (001)LaAlO3

Epitaxial YBa₂Cu₃O₇/La_0.7Ca_0.3MnO₃ (YBCO/LCMO) bi-layers and La_0.7Ca_0.3MnO₃/YBa₂Cu₃O₇ (LCMO/YBCO) bi-layers were grown on (001)LaAlO₃ by pulsed laser deposition, and their microstructures were compared by transmission electron microscopy investigation. In the YBCO(100 nm)/LCMO(150 nm) bi-layers, the LCMO layer consists of columnar grains of ~ 17 nm in diameter and contains mixed orientation domains of [100]_c, [010]_c and [001]_c. The YBCO layer is totally c-axis oriented and the YBCO lattices are tilted − 2.5° to + 2.5° as they grew on the rough surfaces of LCMO columnar grains. For the LCMO(140 nm)/YBCO(140 nm) bi-layers, the LCMO/YBCO interface is sharp and flat. The initial 12-nm thickness of the YBCO layer is composed of c-axis oriented domains, and the upper part of YBCO layer is [100] oriented. The LCMO layer was predominantly [001]_c oriented while [100]_c-oriented domains were occasionally observed.     

MoO3-V2O5-P2O5-Fe2O3玻璃的制备及性能研究

制备了MoO3-V2O5-P2O5-Fe2O3系磷酸盐玻璃,研究了玻璃形成能力、热膨胀系数和抗潮解等性能.结果表明,MoO3-V2O5-P2O5-Fe2O3系统具有较宽的玻璃形成区和较强的玻璃形成能力,当MoO3/V2O5≈1.5时,玻璃形成能力最强.MoO3-V2O5-P2O5-Fe2O3玻璃的热膨胀系数约为60～110×10-7/℃,并且随着Fe2O3含量的增加而逐渐增大.加入适量的Fe2O3能够显著改善MoO3-V2O5-P2O5玻璃的抗潮解性能,在90℃的去离子水中的溶解速率达到8.0×10-9g·cm-2·min-1.     

Structural study of Sr0.3Ba0.7Nb2O6 and La0.030Sr0.255Ba0.700Nb2O6 ceramic systems

Sr_0.3Ba_0.7Nb₂O₆ (SBN) and La_0.030Sr_0.255Ba_0.700Nb₂O₆ (LSBN) ceramic compounds have been prepared using the traditional ceramic method at two different calcination temperatures (900 and 1000 °C) and later sintered both at 1400 °C. A study of the effects of the calcination temperatures and La substitution on the morphological, compositional, and structural properties of SBN and LSBN is presented using scanning electronic microscopy (SEM), energy dispersive spectroscopy (EDS), and X-ray diffraction (XRD) analysis. From Rietveld refinement processes, the XRD patterns were interpreted to evaluate such effects in the structural parameters and the site occupation factors of the heavy metals and oxygen atoms. The effect of the incorporation of La resulted in a 0.25% cell contraction and turned out to be higher than the 0.08% dilation effect produced by the increase of calcination temperature. The La ion with similar effective ionic radius and higher electronegativity is incorporated into the structure occupying the A₁ site just like the Sr ions in the SBN compound. Differences in the site occupation factors between the SBN and LSBN samples lead to substantial changes in the physical properties such as temperature of relative dielectric constant maximum, relative dielectric constant, and dielectric loss, correlated with the distortion and the relative orientation of the oxygen octahedra.     

MgO-Al2O3-SiO2-TiO2-Y2O3玻璃的弹性模量

根据硬盘基板用材料的要求，制备了MgO-Al2O3-SiO2-TiO2-Y2O3高弹性模量玻璃（120GPa)，玻璃的弹性模量随组成的变化服从Makishima-Mackenzie理论，MgO,Al2O3,TiO2,Y2O3等具有较高单位体积离解能的氧化物有利于提高玻璃的弹性模量，但玻璃弹性模量的理论计算值低于测试值，这是因为Makishima-Mackenzie理论没有考虑玻璃内阳离子的具体配位，对MgO,Y2O3堆积密度因子的堆导存在误差，因此利用Makishima-Mackenzie理论发展高弹性模量玻璃时应对MgO,Y2O3等氧化物的计算进行修正。