纳米YSZ：Eu^3＋粉末的制备及光谱研究

本文用化学共沉淀法制备出掺Ｅｕ＾３＋离子的Ｙ２Ｏ３稳定的纳米立方相ＺｒＯ２ 末，并在不同温度下烧结获得不同晶粒度的粉末，分别用Ｘ射线及ＴＥＭ对粉末的晶粒度进行了分析。通过对不同晶粒度的样品进行激发谱和荧光谱的研究表明，随晶粒度减小，ＹＳＺ：Ｅｕ＾３的激发谱峰位有红移现象，其荧光谱的＾５Ｄ０→＾７Ｆ２跃迁有变化，而且各跃迁的强度比也有改变。     

P2O3—B2O3—Al2O3—SrO—BaO玻璃中的Yb^3＋非辐射能量转移下E …

本文研究了共掺Ｅｒ＾３＋／Ｙｂ＾３Ｐ２Ｏ３－Ｂ２Ｏ３－Ａｌ２Ｏ３－ＳｒＯ－ＢａＯ玻璃的能量转移过程。实验中制备了高掺杂Ｂｂ＾３＋离子的双掺Ｅｒ＾＃＋／Ｙｂ＆＾３＋的磷酸盐玻璃样品。在Ｅｒ＾３＋／Ｙｂ＾３＋掺杂比率〉１：１８（ｍｏｌ％）时,观测到了基于Ｙｂ＾３＋离子至Ｅｒ＾３＋离子能量转移下Ｅｒ＾３＋（＾３Ｉ１３／２→＾４Ｉ１５／２）的增强发射和ｂ＾３＋（＾２Ｆ７１／→＾２Ｆ５／２）发射的减弱,当Ｂ     

SiO2气凝胶薄膜中Eu3+离子的跃迁

利用溶胶－凝胶法制得了Ｅｕ＾２＋掺杂ＳｉＯ２气凝胶薄膜,并对其发光及跃迁性质进行了研究。使用原子力显微镜对样品的型貌结构做了观测、采用ＸＲＤ和ＩＯＲ对所得样品的结构进行了研究,测量了样品的激发一发光谱、吸收光谱和时间分辨光谱。通过Ｊｕｄｄ－Ｏｆｅｌｔ理论计算了Ｅｕ＾３＋的＾Ｄ０的辐射跃迁几率,并根据时间分辨光谱研究了＾５Ｄ１的无辐射跃迁几率及弛豫性质。虽然结果与掺Ｅｕ＾３＋的体硅玻璃没有很大差别,     

用溶胶—凝胶法制备的Y2SiO5：Gd,Eu荧光粉的发光性能

用溶胶－凝胶法合成了Ｙ２ＳｉＯ５：Ｇｄ,Ｅｕ红色荧光粉。探讨了烧结工艺对粉体的结构及发光性能的影响。首次报道了搀杂Ｇｄ的Ｙ２ＳｉＯ５：Ｅｕ红色荧光粉的发光性能。研究结果表明,搀杂适当浓度的Ｇｄ,可以显著提高ＹｓＳｉＯ５：Ｅｕ红色荧光粉的发光强度,在Ｙ２ＳｉＯ５基质中,Ｇｄ＾３＋是Ｅｕ＾３＋的优良敏化剂。     

Y^3＋掺杂TiO2复合粒子的光催化活性研究

以钛酸丁酯和氧化钇为原料,采用溶胶－凝胶法研究了Ｙ＾３＋掺杂对ＴｉＯ２光催化活性的影响,通过红外光谱（ＩＲ）分析了ＴｉＯ２复合粒子的结构,结果表明：Ｙ＾３＋掺杂能够显著提高ＴｉＯ２粒子的光催化活性,当掺杂比为１００∶１．５（Ｙ＾３＋外加１．５％）时光催化活性最高,分析了Ｙ＾３＋掺杂ＴｉＯ２粒子光催化活性提高的原因。     

SiO2凝胶玻璃中Eu^＋,Tb^3＋与1,10—邻菲罗啉配合物的原位化学？…

应用原位化学复合方法，将Ｅｕ＾３＋、Ｔｂ＾３＋与，１，１０－邻菲罗啉配合光学均匀复合到ＳｉＯ２凝胶玻璃中，解决了国稀土含氮配合物易水解而难以用溶胶－凝胶工艺将其均匀掺入无机基质的问题。研究了原位配合物的荧光和热学性能。结果表明，由于配合物的形成使稀土离子特征荧光强度显著增加，而无机基质的保护作用则使原位配合物热稳性提高２００℃以上。化学合成纯配合物Ｅｕ（Ｐｈｅｎ）２Ｃｌ３·２Ｈ２Ｏ的高分辨荧光谱表     

含La^3＋的Ni—Zn铁氧体的微观结构和电磁性能

本在Ｎｉ－Ｚｎ铁氧体中掺入Ｌａ２Ｏ３后，材料的电磁性能，温度特性和微观结构所发生的变化，研究了Ｌａ＾３＋离子的掺 杂效应和作用机制。实验表明：Ｎｉ０．４１Ｚｎ０．６０Ｓｎ０．０１Ｃｕ０．０２Ｆｅ２．０４－ＸＬａＸＯ４±δ在ｘ＜０．０１０时，Ｌａ＾３＋离子能细化晶粒；ｘ０．０１０时，Ｌａ＾３＋离子使晶界模糊，晶粒尺寸增大；不同温度区域的电子激活能Ｅρ呈现出明显的差异。Ｌａ＾３＋离子对电阴率ρ的贡献     

溴氧镧铽镝的发光特性及能量传递机理

使用高温常压方法合成了稀土发光材料ＬａＯＢｒ２Ｄｙ＾３＋，Ｔｂ＾３＋，研究了其结构，紫外４主阴极射线激发下的激发与发射光谱，Ｄｙ＾３＋的掺杂可将Ｔｂ＾３＋的＾５Ｄ３能级激光能有地弛豫到＾５Ｄ４能级，从而使５Ｄ４－Ｆ（Ｊ＝０，１）的发射，尤其是＾５Ｄ４－＾７Ｆ５的发射增强，发光亮度提高。     

不同热化学还原LiNbO3∶Ti或Mn晶体杂质电荷态和点缺陷

采用光学吸收和电子顺磁共振（ＥＳＲ）技术表征不同热化学还原ＬｉＮｂＯ３∶Ｔｉ，Ｍｎ（ＬＮ∶Ｔｉ，Ｍｎ）和纯的Ｌｉ／Ｎｂ＝０．９４５一致熔化ＬｉＮｂＯ３（ＬＮ）晶体的热力学还原习性。将ＬＮ∶Ｔｉ（厚度为１ｍｍ）样品放在Ｌｉ２ＣＯ３中、６００℃、保温７ｈ，产生６９０ｎｍ（～１．８ｅＶ，Ｔ＝６７％）和峰值靠近７８５ｎｍ（Ｔ＝７１％）的７７０～８１０ｎｍ光学吸收带，它们分别对应于Ｔｉ＾３＋的＾２Ｔ→＾２Ｅ     

PbF2：Gd,Eu晶体X射线激发的发射光谱

用脱氧剂非真空环境下、Ｓｔｏｃｋｂａｒｇｅｒ方法生长未掺和掺钆和铕的、浓度范围在０．１￣０．２ｗｔ％的ＰｂＦ２：β晶体。本文报导Ｘ射线激发ＰｂＦ２：Ｇｄ晶体的Ｇｄ＾３＋发射。揭示了分别来自＾６Ｐ和＾６Ｉ多重态３１２．５和２７７．４ｎｍ发射带，而＾６Ｄ→＾８Ｓ发射被点阵再吸收。＾６Ｉ的发射强度低于＾６Ｐ，说明＾６Ｐ能级优先占据。室温下以Ｘ射线激发在３６８．９和８１４．５ｎｍ之间观察到１４条Ｅｕ＾３＋     

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.     

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.     

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.     

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.     

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.