掺入Al_2O_3对固体氧化物电解质材料YSZ性能影响的研究

在立方相的钇稳定化氧化锆 [(ZrO2 ) 0 .92 (Y2 O3) 0 .0 8](YSZ)中 ,掺入少许不同量的Al2 O3,研究其对基体材料YSZ的烧结性能、机械强度和导电性能的影响 ,并对其机理进行了分析。实验结果表明 ,掺入Al2 O3能够明显降低电解质烧结温度 ,改善烧结性能。在 130 0℃烧结 1h后 ,少量掺杂Al2 O3的样品晶粒尺寸明显比纯YSZ样品的小 ;从阻抗谱图上可以看出 ,随着Al2 O3含量的增加 ,晶界电阻不断减小 ,在掺杂比例为 4 % (质量分数 )时 ,达到最小点。而后随着Al2 O3含量的增加 ,晶界电阻又呈上升趋势。用纯YSZ和掺 4 % (质量分数 )Al2 O3的材料制成SOFC ,得到伏安特性曲线 ,结果表明 ,掺 4 % (质量分数 )Al2 O3的性能比YSZ好。     

Al2O3掺杂对YSZ固体电解质烧结及电性能的影响

研究了用常规共沉淀法掺杂Al2O3对YSZ固体电解质的烧结及电性能的影响．结果表明：适量的Al2O3能提高YSZ材料的烧结性能，促使其致密化，但过量的Al2O3对材料的致密化不利；同时，材料的晶界电导随Al2O3含量的增大表现出先增大后减小的变化趋势，这与Al2O3对YSZ晶界两方面的不同影响有关，Al2O3偏析于晶界一方面能清除晶界上对氧离子电导不利的SiO2，但另一方面也会降低晶界空间电荷层中的自由氧离子空穴的浓度．     

纳米Al2O3对纳米4YSZ复相陶瓷结构和性能的影响

以纳米4YSZ和纳米Al2O3粉末为原料,对掺少量Al2O3的4YSZ无压烧结体的烧结特性、结构和性能进行了研究.掺适量的Al2O3可降低烧结温度,减缓4YSZ晶粒的长大.少量的交接渗透强化了晶界,烧结体断裂倾向于穿晶断裂,提高了烧结体硬度.     

纳米Al2O3对纳米4YSZ复相陶瓷结构和性能的影响

以纳米4YSZ和纳米Al2O3粉末为原料,对掺少量Al2O3的4YSZ无压烧结体的烧结特性、结构和性能进行了研究。掺适量的Al2O3可降低烧结温度,减缓4YSZ晶粒的长大。少量的交接渗透强化了晶界,烧结体断裂倾向于穿晶断裂,提高了烧结体硬度。     

Al_2O_3掺杂8YSZ固体电解质的烧结及性能研究

通过化学共沉淀法制备Al2O3掺杂的8YSZ固体电解质,并对其进行烧结和性能检测。试验结果表明,掺杂Al2O3有利于降低烧结温度,促使烧结体致密化。并且随着Al2O3掺杂量的增大,晶粒的电导逐渐降低。当Al2O3的加入量少于1.5%(w)时,并没有起到晶界电导改善的作用,反而使晶界性能恶化。     

Y2O3、Al2O3掺杂对CeO2的烧结及电性能的影响

本文采用溶胶-凝胶法制备了不同含量的Y2O3掺杂的CeO2粉体，并在4mol％Y2O3—CeO2粉体中掺入Al2O3，研究了各样品的烧结性能和电性能。结果表明：适量的掺杂Y2O3能提高氧化铈的密度，但Y2O3含量超过4％mol后密度下降。一定量的Al2O3也能提高材料的烧结密度。随着Y2O3含量的增大，CeO2的电导先增大后减小，而掺入Al2O3对材料的电导不利。     

Bi2O3掺量对Li0.45Ni0.2Ti0.1Fe2.25O4铁氧体显微结构及磁性能的影响

采用氧化物法陶瓷工艺,在缺铁配方的基础上,制备不同Bi2O3掺量的Li0.45Ni0.2Ti0.1Fe2.25-δO4(δ=0.06)铁氧体样品。结果表明,添加Bi2O3没有在锂铁氧体中形成杂相,烧结后陶瓷样品物相组成单一,结晶状况良好;适量的Bi2O3能有效改善材料微观形貌,促进锂铁氧体的烧结致密化,有助于提高材料的饱和磁化强度4πMs和剩磁比R,降低矫顽力Hc。Bi2O3掺量为1.5%(质量分数)的样品具有较好的综合性能,表观密度d为4.72g/cm3,饱和磁化强度4πMs为2.3T,剩磁比R为0.853,矫顽力Hc为2.3×102 A/m。     

Y3+共掺杂对掺 Er3+: Al2O3粉末光致发光的增强作用

采用非水性溶胶-凝胶法制备了Y^3＋共掺杂的掺Er^3＋：Al2O3粉末，Er^3＋浓度为0．1和1．0mol％，Er^3＋和Y^3＋浓度比为1：0-10．X射线衍射和光致发光（PL）光谱结果表明：900℃烧结的掺0．1和1．0mol％Er^3＋：Al2O3粉末为具有非晶化特征的γ和θ混合相结构，非晶化趋势随Y^3＋共掺杂浓度增大而增加．掺0．1mol％Er^3＋：Al2O3粉末，PL光谱强度和半高宽随掺Y^3＋浓度增大无明显变化．掺1．0mol％Er^3＋：Al2O3粉末，PL光谱强度和半高宽随掺Y^3＋浓度增大而增加，10mol％Y^3＋共掺杂粉末的发光强度提高50倍，约为掺0．1m01％Er^3＋：Al2O3粉末的10倍，半高宽从77nm增至92nm．Y^3＋共掺杂对较高浓度掺Er^3＋：Al2O3粉末PL性能的增强作用归因于Y^3＋对Er^3＋在基体中的分散和配位结构多样性的提高．     

ZnO掺杂的ZrO2(3Y)纳米复合相材料的中低温电导研究

采用交流阻抗技术对掺纳米ZnO的纳米ZrO2(3Y)复合掺杂材料在473—973K温度范围电导率随ZnO第二相质量分数(0．0％-5．0％(质量分数))的变化关系进行了研究。研究发现掺很少量的纳米ZnO(0．5％-1．0％(质量分数))，纳米ZrO2(3Y)材料晶粒和晶界电阻显著增加，电导率降低，原因在于缺陷缔合效应和晶界偏聚效应的加剧，阻碍了氟空位的迁移。随着ZnO掺入量的增加(＞1．0％(质量分数))，晶界电阻显著减小，晶粒电阻变化不大，总电导率回升，在中低温范围，总电导活化能与晶界电导活化能具有相同的变化趋势。     

Y2O3和纳米AlN协同作用对氮化铝陶瓷烧结性能及热传导的影响

在微米氮化铝粉体中添加含量为4%的Y2O3和不同含量的纳米AlN粉体制备氮化铝陶瓷,研究了Y2O3和纳米AlN协同作用对微米氮化铝陶瓷烧结性能和热传导性能的影响。结果表明,Y2O3优先与纳米AlN粉体表面的Al2O3反应生成活性较高的第二相Al5Y3O12,相比于Y2O3与微米AlN粉体表面Al2O3反应生成的Al5Y3O12,具有更低的熔化温度及更好的流动性;同时,纳米AlN粉体的高比表面能也促进氮化铝陶瓷的致密化进程。二者的协同作用有效地促进氮化铝陶瓷的致密烧结,改善第二相的微观分布,从而能在较低的烧结温度下获得具有较高热导率的氮化铝陶瓷。当Y2O3和纳米AlN粉体的添加量(质量分数)分别为4%和1.5%时,在1800℃烧结得到的氮化铝陶瓷密度为3.26 g·cm-3,第二相以连续相的形式分布于氮化铝晶界处,热导率为151.75 W/(m.K)。     

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。