纳米片钠铝石结构KAl(OH)2CO3的水热合成

用水热法制备出了纳米级粒径的纤维状KAl(OH)2CO3,并研究了不同水热反应条件对KAl(OH)2CO3的形成、颗粒度以及形态的影响.研究表明,不同条件下合成的晶粒均呈纤维状,随着温度的升高,长度和粒径均有所增大.在120℃制备得到的纤维平均直径为30nm,且分布均匀;KHCO3和Al(OH)3之比对KAl(OH)2CO3的形貌有显著的影响,KHCO3用量越大,晶粒直径越细;随着介质碱性的增强,晶粒直径在pH为9.5时出现极小值,且粉体的均匀性最好.在特定的反应体系中,当反应时间达到2h后,合成反应基本达到平衡,进一步延长合成时间对粉体的形貌和颗粒尺寸没有明显的影响.     

纳米羟基磷灰石粉体的水热合成

采用Ca(NO3)2·4H2O和(NH4)3PO4·3H2O作为反应前驱物,通过水热合成颗粒尺寸在100nm以下的短棒状或针状HA晶体.X射线衍射(XRD)、透射电镜(TEM)和红外光谱(FTIR)分析讨论水热温度、反应时间、表面活性剂和烧结与物相组成、晶粒尺寸和晶体形貌的关系.实验结果表明升高反应温度和延长反应时间有利于HA的生成;表面活性剂有助于改善粉体的分散性能;烧结能提高晶体的结晶程度,但粉体易团聚,当温度高于800℃时HA发生分解.     

醇-水法制备纳米晶NiO粉体

Ni(NO3 ) 2 ·6H2 O和NH4HCO3 在醇 水溶液中反应合成NiCO3 · 2Ni(OH) 2 ·2H2 O前驱体 ,经煅烧后得到大约 10nmNiO粉体。同传统的水溶液法相比 ,醇 水法得到的NiO粉体粒径尺寸小、分布范围窄和团聚少 ,PEG的添加能够减少团聚     

纳米片钠铝石结构KAl(OH)2CO3的水热合成

用水热法制备出了纳米级粒径的纤维状KAl(OH)2CO3，并研究了不同水热反应条件对KAl(OH)2CO3的形成、颗粒度以及形态的影响．研究表明，不同条件下合成的晶粒均呈纤维状，随着温度的升高，长度和粒径均有所增大．在120℃制备得到的纤维平均直径为30nm，且分布均匀；KHCO3和A1(OH)3之比对KAl(OH)2CO3的形貌有显著的影响，KHCO3用量越大，晶粒直径越细；随着介质碱性的增强，晶粒直径在pH为9．5时出现极小值，且粉体的均匀性最好．在特定的反应体系中，当反应时间达到2h后，合成反应基本达到平衡，进一步延长合成时间对粉体的形貌和颗粒尺寸没有明显的影响．     

纳米Ni0.5Zn0.5Fe2O4铁氧体的制备及电磁损耗特性研究

采用NH4 HCO3与FeCl3·6H2O、Zn(NO3)2·6H2O、Ni(NO3)2·6H2O进行室温固相反应制得Fe(OH)3、Zn3(OH)4CO3·H2O、Ni3(OH)4CO3·4H2O混合前驱物,先经微波加热,再热分解制得纳米粉体.利用激光粒度分析仪、XRD、SEM和TEM对分解产物进行了表征,获得了形貌为球形、颗粒分布均匀、平均粒度为62nm、尖晶石结构的纳米Ni0.5Zn0.5Fe2O4复合铁氧体粉体.经测试样品的相对介电常数和相对磁导率后,发现该纳米铁氧体粉体在100～1800MHz内具有良好的电损耗和磁损耗性能.     

钛酸铋纳米粉体的水热合成研究

讨论了水热合成条件(原料种类、摩尔配比、反应温度和晶化时间)对水热法制备钛酸铋粉体结构和形貌的影响,以Bi(NO3)3·5H2O和TiCl4为原料,NaOH为矿化剂,在180～230℃和2～12h的水热条件下,制备出Bi4Ti3O12纳米粉体.XRD结果表明它是典型的层状钙钛矿结构.TEM观察表明,Bi4Ti3O12纳米晶是方形片状的,无团聚,晶粒边长分布为80～250nm,平均长度约200nm.     

低温碳热还原法合成氮化铝陶瓷超细粉末

采用硝酸盐-有机物低温燃烧反应溶胶-凝胶工艺,以硝酸铝（Al（NO3）3·9H2O）、葡萄糖（C6H12O6·H2O）、尿素（CO（NH2）2）为原料,制备出粒度细小、混合均匀的铝源和碳源的混合前驱物,然后以该前驱物为原料进行碳热还原反应制备氮化铝粉末.研究表明,该前驱物具有较高的反应活性,氮化反应速率快,1550℃时仅用90min即可实现完全转化,SEM分析结果表明合成粉末为粒度分布均匀的纳米级（～100nm）粉末.     

湿化学法制备 Y2O3纳米粉及透明陶瓷

以Y(NO3)3溶液和NH3·H2O为原料,制备了Y2O3纳米粉体.先驱沉淀物的化学组成为Y2(OH)5NO3·H2O.研究了pH值及滴加过程对先驱沉淀物形貌及Y2O3产物烧结性的影响.正向滴定,pH值较低时(pH=7.9),先驱沉淀物为片状结构;pH值较高时(pH=10.0),先驱沉淀物片层状结构特性减轻,并且颗粒变的细小.反向滴加时,片层状结构特征消失,主要为块状晶粒.先驱沉淀物为片状结构时,得到的粉体活性较高.添加适量的(NH4)2SO4能够减轻Y2O3粉体的团聚,沉淀的同时控制pH值在9以下,所得到的粉体具有更好的烧结性能.采用得到的Y2O3纳米粉,不加入任何烧结助剂,经1700℃真空烧结4h得到了透明Y2O3陶瓷.     

Ca2Co2O5化合物的制备及热电性能的研究

以Co(NO3)2·6H2O,Ca(NO3)2·4H2O为原料,Na2CO3为沉淀剂,采用化学共沉淀法和放电等离子烧结(SPS)制备了Ca2Co2O5化合物.采用TG-DTA、XRD和SEM等手段对前驱体的热分解过程,样品的物相以及形貌进行了表征,测试了Ca2Co2O5的热电性能.实验结果表明沉淀前驱物经850℃预烧8 h后,利用SPS 850℃,压力30MPa保温5min,制备了纯相Ca2Co2O5化合物.该化合物的电阻率和热导率均随温度的升高而降低,800℃时,热电性能优值(ZT)为0.12.     

一维纤维状α-Al2O3粉体的水热-热解法制备与表征

以Al(NO3)3·9H2O、尿素为原料,以PEG2000为表面活性剂,采用水热-热解法合成纤维状氧化铝粉体。用XRD、SEM对产物进行表征,研究了不同水热时间、pH值、硝酸铝浓度、PEG2000添加量及铝源等因素对纤维状α-Al2O3粉体结晶状况、晶粒尺寸、晶体形貌的影响,分析了合成反应机理。实验结果表明:PEG2000添加量是影响反应体系得到纤维形貌产物的关键。     

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.     

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.     

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.     

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.     

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.     

静电纺丝法制备的Co0.6Ni0.3Cu0.1Fe2O4和Co0.6Ni0.3Zn0.1Fe2O4纳米纤维的结构及磁性能

采用静电纺丝技术制备出表面光滑、直径均匀的Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4/PVP和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4/PVP纳米纤维前驱丝,经500~900℃煅烧后得到Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维。用TG-DSC、XRD、SEM及VSM现代测试分析手段对Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维的结构、形貌及磁学性能进行测试表征。结果表明:在空气气氛中经500~900℃煅烧后可得到纯尖晶石相、结晶度良好的纳米纤维或短纤维;当温度为700℃时,Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4和Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维的形貌细长而光滑且直径相对均匀,大约为80nm;此时Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4纳米纤维则保有较高的剩磁比(M_r/M_s)及矫顽力,分别为0.56和1 088.87Oe。在500℃、600℃、700℃、800℃、900℃煅烧后,Co_(0.6)Ni_(0.3)Zn_(0.1)Fe_2O_4纳米纤维的饱和磁化强度分别比Co_(0.6)Ni_(0.3)Cu_(0.1)Fe_2O_4纳米纤维增大了14.5%、7%、16%、10.7%、8%,而矫顽力则分别降低了38%、51%、50%、46%、46.7%。两种纳米纤维的饱和磁化强度及矫顽力存在差异,为CoNi铁氧体在电磁方面的应用提供了很好的参考。