添加Y2O3-Dy2O3的AlN陶瓷的烧结特性及显微结构

本文探索了以自蔓延高温（ＳＨＳ）法合成并经抗水化处理的ＡｌＮ粉为原料,以Ｙ２Ｏ３－Ｄｙ２Ｏ３作为助烧结剂的ＡｌＮ陶瓷的烧结特性及显微结构,结果表明,晶界处存在Ｄｙ４Ａｌ２Ｏ９、Ｙ３Ａｌ２Ｏ９、ＤｙＡｌＯ３、Ｄｙ２Ｏ３和ＤｙＮ等第二相物质,随烧结温度变化,第二相的种类、数量和分布不同,显微结构也随之变化,从而影响ＡｌＮ的热导率,在１８５０℃下,可获得热导率为１４８Ｗ／ｍ·Ｋ的ＡｌＮ陶瓷。     

AlOOH对Al2O3直接凝固注模成型坯体强度等性能影响

为了改善直接注模成型（ＤＣＣ）氧化铝的坯体性能，在Ａｌ２Ｏ３－ＤＣＣ过程中加入ＡｌＯＯＨ本文详细研究了Ａｌ２Ｏ３＋ＡｌＯＯＨ体系的湿坯性能，干燥行为及烧结致密化过程，结果表明，少量ＡｌＯＯＨ加入可显著提高Ａｌ２Ｏ３的湿坯抗压强度和弹性模量，当ＡｌＯＯＨ体积含量〈３．０％时对干燥过程没有影响，干燥坯体经无压烧结后可获得烧结密度达３．９７ｇ／ｃｍ＾３（９９．７％ＴＤ）。显微结构均匀的α－Ａｌ２Ｏ３相。     

Al2O3的粉末特征对β-Al2O3烧结性能的影响

研究了Ａｌ２Ｏ３原料在不同热处理条件下的相组成和颗粒形貌以及Ａｌ２Ｏ３粉末特征对Ｎａ－β″－Ａｌ２Ｏ３烧结性能的影响，实验表明，只有α－Ａｌ２Ｏ３才能烧结成致密的β″－Ａｌ２ｏ３陶瓷。     

CaO-Y2O3添加剂对AlN陶瓷显微结构及性能的影响

研究了掺杂ＣａＯ－Ｙ２Ｏ３热压烧结和常压烧结ＡｌＮ陶瓷的性能和显微结构．结果表明：热压烧结ＡｌＮ陶瓷的第二相为Ｙ３Ａｌ５Ｏ１２，常压烧结ＡｌＮ陶瓷的第二相为Ｙ３Ａｌ５Ｏ１２和Ｃａ３Ｙ２Ｏ６；热压烧结ＡｌＮ的第二相体积百分数和晶格氧含量均低于常压烧结；热压烧结ＡｌＮ陶瓷的微观结构良好，其热导率达到２００Ｗ／ｍ·Ｋ．     

γ-Al2O3纳米粉对氧化铝纤维烧结行为的影响

研究了纳米γ－Ａｌ２Ｏ３粉末对化铝纤维烧结行为的影响,在纤维挤在坟成型过程中,纳米粉体填入到微米颗粒形成的孔隙中,当另入量为４０ｗｔ％时,纤维素相对密度由６５％提高到８０％,由于成型密度高、气孔分布窄、孔径小而有利于烧结,在较低的烧结温度下可以达到理论密度,全部采用纳米γ－Ａｌ２Ｏ３粉挤压纤维烧结后具肋交大的径向收缩率,在１２００℃烧结即可达到完全致密。     

YAG- Al2O3纳米复合材料的制备和力学性能

本文介绍了用化学共沉淀和在适当温度下煅烧以直接制备ＹＡＧ－Ａｌ２Ｏ３纳纳米复合粉体的新方法。ＸＲＤ结果表明,所得粉体具纯的ＹＡＧ和α－Ａｌ２Ｏ３相,因此其化学组成符合配料的组分设计,用本方法制备的２５ｖｏｌ％ＹＡＧ－Ａｌ２Ｏ３复合粉体经热压烧结,所得的致０密体材料为晶内型纳米复合材料,其抗弯强度达６１２ＭＰａ,断裂韧性为４．５４ＭＰａｍ＾－１／２,都比单相Ａｌ２Ｏ３陶瓷有大幅度提高。     

Naβ/β″-Al2O3膜的制备与电学性能研究

通过ＭｇＡｌ２Ｏ４－α－Ａｌ２Ｏ３复合相陶瓷基体与Ｌｉ２Ｏ，Ｎａ２Ｏ气氛的反应制备了Ｌｉ２Ｏ和ＭｇＯ共同稳定的Ｎａβ／β″－Ａｌ２Ｏ３膜，相分析的结果表明，反应温度是决定膜中β／β″Ａｌ２Ｏ３相形成速率的主要因素，当温度低于１１００℃时，α－Ａｌ２Ｏ３基体不能转化为β／β″－Ａｌ２Ｏ３基体中的ＭｇＡｌ２Ｏ４可以促进膜的形成，并降低膜的形成温度，交流复阻抗谱和四极法测量的结果表明，复合基体表面形成的     

Al—Al2O3—玻璃复合材料的制备与性能

采用无压烧结工艺，制备了Ａｌ－Ａｌ２Ｏ３－玻璃复合材料。研究了Ａｌ－玻璃，Ａｌ２Ｏ３－玻璃的润湿性。发现玻璃能促进Ａｌ与Ａｌ２Ｏ３结合；Ａｌ－Ａｌ２ｏ３－玻璃复合材料具有良好的强度和耐磨损性能。     

Al—Al2O3粉末成形体烧结性的研究

分析研究了金属Ａｌ在１０００℃左右温度下的存在状态以及Ａｌ２Ｏ３上浸润性问题，讨论了Ａｌ－Ａｌ２Ｏ３两相末成形的烧结性能及助烧剂，烧结气氛对材料烧结性能的影响。结果表明，由于金属Ａｌ的活泼性以及生成的Ａｌ２Ｏ３膜的稳定性和金属Ａｌ对Ａ２Ｏ３表面浸润性差等原因决定了Ａｌ－Ａｌ２Ｏ３粉未成形体在１０００℃时的烧结性能极差。     

SiC-ZrO2(3Y)-Al2O3纳米复相陶瓷的力学性能和显微结构

本文介绍用非均相沉淀方法制备的纳米ＳｉＣ－ＺｒＯ２（３Ｙ）－Ａｌ２Ｏ３复合粉体经放电等离子超快速烧得到晶内型的纳米复相陶瓷,超快速烧结的升温速率为６００℃／ｍｉｎ,在烧结温度不保温,迅即在３ｍｉｎ内冷却至６００℃以下。     

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.     

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.     

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.     

Vapour-liquid equilibria in the ternary mixtures N2---CH4---C2H6 and N2---C2H6---C3H8

A systematic study was performed with mixtures consisting of N₂, CH₄, C₂H₆ and C₃H₈, to investigate experimentally phase equilibria and caloric properties and to test the accuracy of thermodynamic correlations. The first part of this Paper reports results of T---p---x---y measurements on ternary systems in the range 20 < p < 120 bar and 140 < T < 220 K. The results are compared with data calculated by generalized equations of state.     

PbSbBiS4-Sb2S3 and PbSbBiS4-Bi2S3 joins in the PbS-Sb2S3-Bi2S3 system

Phase equilibria along the PbSbBiS₄-Sb₂S₃ and PbSbBiS₄-Bi₂S₃ joins of the PbS-Sb₂S₃-Bi₂S₃ system have been studied for the first time using differential thermal analysis, X-ray diffraction, microstructural analysis, microhardness tests, and density measurements, and the phase diagrams of the joins have been mapped out. The joins are shown to be pseudobinary with limited series of terminal solid solutions. The solid solutions are p-type semiconductors.     

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.     

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.     

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.