Li1+2x+yAlxNdyTi2-x-ySixP3-xO12系统的锂快离子导体研究

Ｌｉ１＋２ｘ＋ｙＡｌｘＮｄｙＴｉ２－ｘ－ｙＳｉｘＰ３－ｘＯ１２锂快离子导体可以用精选的天然高岭石Ａｌ４「Ｓｉ４Ｏ１０」（ＯＨ）８为起始原料，经与Ｌｉ２Ｃｏ３、ＴｉＯ２、ＮＨ４Ｈ２ＰＯ４进行高温（８００－１０００℃固相反应约２０ｈ而制得，一个空间群属于Ｒ３Ｃ的固溶体导电相可在ｙ＝０．５，ｘ≤０．３和ｙ＝１．０，ｘ≤０．４的组成范围内发现，该盯具有较好的电导性较低的活化能，起始组成ｙ＝１．０，ｘ＝０．     

Na2Mo0.1S0.9O4(α)-In2(SO4)3体系的导电性、相关系与红外光谱研究

本文报道了应用Ｘ射线衍射，差热分析，ＩＲ光谱及电测量技术对Ｎａ２Ｍｏ０．１Ｓ０．９Ｏ４（α）－Ｉｎ２（ＳＯ４）３体系的研究结果，讨论Ｉｎ２（ＳＯ４）３对Ｎａ２Ｍｏ０．１Ｓ０．９Ｏ４的导电性及相存在形式的影响。     

多孔La0.6Sr0.4Co0.2Fe0.8O3-δ的制备及表征

多孔Ｌａ０．６Ｓｒ０．４Ｃｏ０．２Ｆｅ０．８Ｏ３－δ陶瓷具有一定的强度、良好的透气和电传导性能,可用于中温ＳＯＦＣ阴极支撑和氧分离膜活性支撑体。本文用固相反应法制备了多孔Ｌａ０．６Ｓｒ０．４Ｃｏ０．２Ｆｅ０．８Ｏ３－δ陶瓷。考察了烧结条件１成型压力有机添加剂量对孔隙率和孔径的影响,研究发现气体渗透随机孔隙率线性增长,电导率随孔隙率的增大而下降,并满足关系式σ＝σ０（１－Ｐ）＾３．１。     

Na2Mo0.1S0.9O4（α）—Pr2（SO4）3二元系的相关系与导电性

应用差热分析、Ｘ射线粉末衍射及电测量技术对Ｎａ２Ｍｏ０．１Ｓ０．９Ｏ４（α）－Ｐｒ２（ＳＯ４）３体系进行了研究，结果表明，在Ｎａ２Ｍｏ０．１Ｓ０．９Ｏ４相中加入少量的Ｐｒ２（ＳＯ４）３就可以形成完全固熔体，且无任何相变存在，当Ｐｒ２（ＳＯ４）３含量达到４ｍｏｌ％时，电导率较纯Ｎａ２Ｍｏ０．１Ｓ０．９Ｏ４提高两个数量级（５５３Ｋ时，σ＝１．０９×１０＾－３Ｓｃｍ＾－１），同时还证明了该类导体的导电机     

大功率CO2激光熔凝稳定ZrO2

利用大功率ＣＯ２激光熔凝稳定ＺｒＯ２高温快离子导体获得成功．报导了激光熔凝的原理、工艺过程及熔凝后样品的微观分析等研究结果．激光熔凝的ＣＳＺ和ＭＳＺ快离子导体样品在温度为１０００℃时的电导率达到２×１０－２Ω－１ｃｍ－１量级．     

O＋HO2反应碰撞的理论研究

使用多体项展式分析势能函数，研究了Ｏ＋ＨＯ２反应碰撞的经典轨迹，指出存在二个反应通道，即（１）Ｏ＋ＨＯ２→ＯＨ＋Ｏ２和（２）Ｏ＋ＨＯ２→ＨＯ２＋Ｏ。在室温下，求得反应（１）的近似速度常数为（４．１±０．０６）×１０＾－１１ｃｍ＾３·ｍｏｌｃｃｕｌｅ＾－１·Ｓ＾－１，与实验值（５．４±０．９）×１０＾１１符合甚好；反应（２）的速度常数为５．４×１０＾－１３。对反应（１），总能量的７２．５％分配于产物     

掺SrLi1／4Nb3／4O3的SrTiO3缺陷化学研究

利用Ｈ２／Ｈ２Ｏ体系获得不同的氧分压,上电极法 掺杂ＳｒＬｉ１／４Ｎｂ３／４Ｏ３的ＳｒＴｉＯ３瓷体在８００－１２００℃,Ｐｏ２＝１０＾１７－１０＾５Ｐａ的电导率。通过ｌｏｇＰｏ２－ｌｏｇσ图,计算出半导化活化焓约为２８７．７ｋＪ／ｍｏｌ,讨论了ＳｒＬｉ１／４Ｎｂ３／４Ｏ３掺杂的ＳｒＴｉＯ３在不同氧分压区域的主ｎ型半导体化向ｐ型半导化转变的特点。     

掺杂BaCeO3和SrCeO3在氧,氢及水气气氛下的电导性能

掺杂碱土金属铈酸盐系统：ＭＣｅ１－ｘＲｘＯ３－ｘ／２（Ｍ＝Ｂａ，Ｓｒ；Ｒ＝Ｙｂ，Ｙ，Ｇｄ，Ｌａ；ｘ＝０．０１～０．１０）可由固相反应制得单相化合物，Ｘ射线衍射分析表明，掺杂元素及掺杂量对掺杂ＢａＣｅＯ３和ＳｒＣｅＯ３的晶体结构影响不大。用复数阻抗谱研究了在氧、氢、水气气氛下的电导性能。在各种气氛下ＭＣｅ０．９５Ｙｂ０．０５Ｏ２．９７５（Ｍ＝Ｂａ，Ｓｒ）的电导率最大。根据测试结果，结合缺陷化学理论讨     

纳米ZrO2/(1-n)SiO2-nAl2O3介孔复合作的制备与光致发光

采用溶胶－凝胶法和超临界干燥技术制备了（１－ｎ）ＳｉＯ２－ｎＡｌ２Ｏ３（ｎ＝０、０．０１、０．１）混合气凝胶体系，并以此作为载体，成功地将纳米ＺｒＯ２粒子组装到（１－ｎ）ＳｉＯ２－ｎＡｌ２Ｏ３介孔体系中，而形成纳米ＺｒＯ２／（１－ｎ）ＳｉＯ２－ｎＡｌ２Ｏ３介孔复合材料。光致发光光谱研究表明，室温下以３１６ｎｍ（３．９２ｅＶ）波长激发时，纳米ＺｒＯ２粒子５４０ｎｍ（２．３０ｅＶ）荧光峰，在介孔复合体     

LaCaO3基固体电解质在SOFC中的应用

对锶镁掺杂的镓酸镧（Ｌａ０．９Ｓｒ０．１Ｇａ０．８Ｍｇ０．２０３,简写为ＬＳＧＭ１０２０）电解质的电化学性能进行了初步的研究,并以它为电解质,Ｎｉ－ＣｅＯ２为阳极,Ｌａ（Ｓｒ）ＭｎＯ３为阴极制作了ＳＯＦＣ测试电池。对Ｈ２－ｏ２电池的伏安特性进行了测试。用能量损失谱（ＥＤＳ）研究了测试电池断面各种元素的分布情况。结果表明,本研究中得到的ＬＳＧＭ电解质有中温离子电导率高,高温电导率偏低的特点。在不同的温度范围氧离子迁移数均接近于１。测试电池的最大输出功率密度为６７．７ｍＷ／ｃｍ＾２,最大电流密度为１２６．３ｍＡ／ｃｍ＾２。ＥＤＳ结果显示,作为电解质主要元素之一的Ｇａ发生了从电解质到阳极的扩散过程,而作为阳极主要成分之一的Ｎｉ也扩散到了电解质中。这可能是导致测试电池最大输出功率和最大电流密度偏低的主要原因。可以认为,     

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.     

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.     

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.     

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.     

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.     

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。     

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.     

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.     

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.