退火温度对Mm（NiCoMnAl）5/5wt%Mg2Ni储氢合金结构和电化学性能的影响

采用二步熔炼法制备了Mm(NiCoMnAl)5/5%(质量分数)Mg2Ni复合储氢合金,并对其在不同温度(1023、1123和1223K)下进行退火热处理10h。用X射线衍射(XRD)、扫描显微镜(SEM)和电化学测试方法研究了退火温度对合金结构和电化学性能的影响。结果表明,铸态Mm(NiCoMnAl)5/5%(质量分数)Mg2Ni复合合金由LaNi5相和少量的Mg2Ni相组成,而退火态合金由LaNi5相和(La,Mg)Ni3新相组成。合金的最大放电容量和高倍率放电性能随退火温度的升高呈现出先增强后减弱的变化规律,其中退火温度为1023K时,合金电极的上述性能均达到最佳。合金的容量保持率随退火温度的升高而单调地增大,60次充放电循环后容量保持率从铸态合金的86.6%增大到退火合金(1223K)的92.4%。     

退火温度对Mm(NiCoMnAl)5/5%(质量分数)Mg2Ni储氢合金结构和电化学性能的影响

采用二步熔炼法制备了Mm(NiCoMnAl)5/5%(质量分数)Mg2Ni复合储氢合金,并对其在不同温度(1023、1123和1223K)下进行退火热处理10h。用X射线衍射(XRD)、扫描显微镜(SEM)和电化学测试方法研究了退火温度对合金结构和电化学性能的影响。结果表明,铸态Mm(NiCoMnAl)5/5%(质量分数)Mg2Ni复合合金由LaNi5相和少量的Mg2Ni相组成,而退火态合金由LaNi5相和(La,Mg)Ni3新相组成。合金的最大放电容量和高倍率放电性能随退火温度的升高呈现出先增强后减弱的变化规律,其中退火温度为1023K时,合金电极的上述性能均达到最佳。合金的容量保持率随退火温度的升高而单调地增大,60次充放电循环后容量保持率从铸态合金的86.6%增大到退火合金(1223K)的92.4%。     

添加Si对La-Mg-Ni系A2B7型电极合金循环稳定性的影响

为了改善La-Mg-Ni系A2B7型电极合金的电化学循环稳定性,在合金中添加少量Si。采用真空感应熔炼制备了La0.8Mg0.2Ni3.3Co0.2Si x(x=0~0.2)电极合金,并将部分合金在真空条件下,温度为900、950、1000和1050℃下进行了退火处理。用XRD、SEM分析了铸态及退火态合金的微观结构,测试了铸态及快淬态合金的电化学循环稳定性。结果表明,铸态及快淬态合金均具有多相结构,包括两个主相(La,Mg)2Ni7和LaNi5及一个残余相LaNi3。添加Si使LaNi5相增加而(La,Mg)2Ni7相减少。合金的电化学循环稳定性随Si含量的增加而增加,当Si含量x从0增加到0.2时,铸态合金100次充放循环后的容量保持率(S100)从64.2%增加到73.1%,而950℃退火态合金的S100值从80.3%增加到93.7%。     

快淬La-Mg-Ni系贮氢电极合金的结构与电化学性能

铸态及快淬态La2Mg(Ni0 85Co0.15)9Cr01贮氢电极合金主要由(La,Mg)Ni3相(PuNi 3型结构),LaNi5相以及少量的LaNi2相组成,各相的含量与淬速有关.与铸态合金相比较,快淬态合金放电平台电压降低,快淬使合金的循环寿命都有不同程度的提高.铸态和快淬态合金均具有良好的活化性能.     

相组成对La0.75 Mg0.25 Ni3.5储氢合金电化学性能的影响

La-Mg-Ni基超晶格储氢合金与传统AB5型合金相比,具有优越的电化学容量,近年来受到研究者们的广泛关注,但是其合金相组成复杂,综合电化学性能尤其是循环稳定性有待提高.本工作通过将A2B7型La0.75Mg0.25Ni3.5合金在1203 K下退火40 h,制备了只含有(La,Mg)2Ni7和(La,Mg)5Ni19超晶格结构的合金,并研究了相转变对合金电化学性能的影响.研究表明,铸态合金含有(La,Mg)Ni3、(La,Mg)2Ni7和(La,Mg)5 Ni9超晶格相以及LaNi5相,在退火过程中,位于相图相对边缘位置的LaNi5相和(La,Mg)Ni3相消失,得到了只含有(La,Mg)2 Ni7和(La,Mg)5 Ni9超晶格的双相合金.超晶格相总量的增加伴随着元素组成的均匀化和应力的降低,这不但有效提高了合金的储氢容量,而且减轻合金在充/放电循环过程中的粉化和氧化,显著提高合金电极的循环稳定性.合金电极的最大放电容量由铸态的355 mAh·g-1提高到退火态的367 mAh·g-1,100周的循环稳定性由57.97％显著提高到81.47％.但是由于合金中的缺陷和晶界的减少,合金的高倍率放电性能有所降低.     

La0.7Mg0.3Ni2.65Co0.75-xMn0.1Six储氢电极合金的结构和电化学性能

系统研究了Si部分替代Co对La0.7Mg0.3Ni2.65Co0.75Mn0.1储氢电极合金结构和电化学性能的影响。XRD结果显示,随着Si替代量的增加,合金中(La,Mg)Ni3相的丰度逐渐降低,而LaNi5相的丰度逐渐增加,且含Si合金中出现了La2Ni7相。电化学测试表明,Si部分替代Co降低了合金的放电容量,但显著提高了其循环稳定性,改善了其高倍率放电性能。其中Si替代量x=0.15时合金的综合性能较好,合金最大放电容量323mAh/g,75次循环后的容量保持率约为71.9%,1250mA/g电流放电时的HRD可达55%。     

Pr替代La对La-Mg-Ni系A_2B_7型电极合金微观结构及循环稳定性的影响

为了改善La-Mg-Ni系A2B7型电极合金的电化学循环稳定性,用Pr部分替代合金中的La,并用熔体快淬技术制备了La0.75-xPrxMg0.25Ni3.2Co0.2Al0.1(x=0、0.1、0.2、0.3、0.4)电极合金。用XRD、SEM、TEM分析了铸态及快淬态合金的微观结构,测试了铸态及快淬态合金的电化学循环稳定性,研究了Pr替代La对合金微观结构及循环稳定性的影响,探讨了合金电极在电化学循环过程中的失效机理。结果表明,铸态及快淬态合金均具有多相结构,包括2个主相(La,Mg)Ni3及LaNi5和一个残余相LaNi2。Pr替代La使(La,Mg)Ni3明显增加而LaNi5减少。电化学测试的结果表明,合金的循环稳定性随Pr替代量的增加而增加。导致合金电极失效的主要原因是电极表面被电解液剧烈腐蚀以及合金电极在电化学循环过程中的粉化。     

熔体快淬对La0.75-xZrxMg0.25Ni3.2Co0.2Al0.1(x=0～0.2)电极合金循环稳定性的影响

为了改善La-Mg-Ni系A287型电极合金的电化学循环稳定性,用Zr部分替代合金中的La,并用熔体快淬工艺制备了La0.75-xZrxMg0.25Ni3.2Co0.2Al0.1(x=0、0.05、0.1、0.15、0.2)电极合金.用XRD、SEM、TEM分析了铸态及快淬态合金的微观结构,测试了铸态及快淬态合金的电化学循环稳定性,研究了快淬工艺及Zr替代La对合金循环稳定性的影响,探讨了电极合金的失效机理.结果表明,铸态及快淬态合金均具有多相结构,包括两个主相(La,Mg)Ni3及LaNi5和一个残余相LaNi2.快淬处理及Zr替代La可以显著的改善舍金的电化学循环稳定性.导致合金失效的主要原因是电极表面被电解液剧烈腐蚀以及合金电极在电化学循环过程中的粉化.     

铸态及快淬态La2Mg(Ni0.85Co0.15)9Bx(x=O～O.2)贮氢合金的微观结构与电化学容量

用铸造及快淬工艺制备了La-Mg-Ni系(PuNi3型)贮氢合金La2Mg(Ni0.85Co0.15)9Bx(x=0,0.05,0.1,0.15,0.2),分析测试了铸态及快淬态合金的微观结构与电化学容量,研究了硼及快淬工艺对合金微观结构及电化学容量的影响.结果表明,铸态合金具有多相结构,包括(La,Mg)Ni3相(PuNi3型)、LaNi5相,一定量的LaNi2相和微量的Ni2B相,经快淬处理后Ni2B相消失.硼的加入对铸态及快淬态合金的容量产生不同的影响,铸态合金的容量随硼含量的增加而单调下降,而快淬态合金的容量随硼含量的增加有一极大值.快淬处理对含硼及不含硼合金的容量也有不同的影响,随淬速的增加,不含硼合金的容量单调下降,而含硼合金的容量可以获得一个极大值.     

La2-xMgxNi7.0(x=0.4,0.5,0.6,0.7,0.8)贮氢合金结构和电化学性能的研究

用高频感应熔炼的方法制备了La2-xMgxNi7.0(x=0.4,0.5,0.6,0.7,0.8)贮氢电极合金,采用x-ray衍射和XRD粉末衍射全谱拟合分析方法及电化学方法系统研究了随Mg含量的增加,该类合金相结构和电化学性能的变化规律,以及合金在不同退火温度(1123K,1203K,1253K)和不同退火时间(24h,72h,144h)下相结构和微观组织及电化学性能的变化规律.实验结果表明,该类合金由(La,Mg)2Ni7相(Ce2Ni7型结构)、LaNi5(CaCu5型结构)相、(La,Mg)Ni3相(PuNi3型结构)及少量未知相组成.随Mg含量的增加,电极电化学放电容量呈先升高后降低趋势,当x=0.6时达到最大值389.87mAh/g;当Mg含量进一步增加时,电化学放电容量迅速降低,x=0.8时电化学放电容量为188.34mAh/g;随Mg含量的增加,合金组织中(La,Mg)Ni3相和LaNi5相增多.退火处理很大程度上消除了LaNi5相,高温退火有利于(La,Mg)2Ni7相的生成,低温退火有利于(La,Mg)Ni3相生成.退火时间的延长对合金相结构影响不明显,但提高了合金组织均匀性,同时使电化学放电容量降低.不同的退火温度和退火时间对未知相影响不明显.本文研究表明,退火温度对(La,Mg)2Ni7合金相结构有重要影响,Mg含量是影响合金相结构和电化学放电容量的关键.     

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.     

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。