溶胶-凝胶法制备Li（MoO4）2：Eu及表征

用溶胶-凝胶法制备了平均粒径为2～3μm的小颗粒、高亮度的Li（2-x）（MoO4）2：Eu系列钼酸盐红色荧光体。用XRD、SEM、粒度分析和分子荧光光度计对荧光体进行了表征和研究。常规的固相反应合成Li（2-x）（MoO4）2：Eux系列红色荧光粉需要在900℃以上的高温才能够形成均一的固溶体，而采用溶胶-凝胶法制取，在700℃就可以形成均一的单相Li（2-x）（MoO4）2：Eux，在750℃就可得到发光亮度最高的荧光体。其亮度是常规固相反应于900℃制得的荧光体的124％。采用溶胶-凝胶法制取Li（2-x）（MoO4）2：Eux系列，可以在相当宽的实验条件范围内得到小粒径、窄分布和高亮度的荧光体，具有良好的颗粒形貌。     

白光LED用红色荧光粉的制备及性能研究

采用溶胶-凝胶法合成了可用于395 nm及465 nm激发的Ca1-2xBxEu MoO4 (B=Li+,Na+,K+)红色荧光粉.用XRD和荧光光谱对其结构、发光性能进行了表征,并就不同电荷补偿对其发光性能的影响进行了分析.同时研究了煅烧温度及Eu3+浓度对所得荧光粉发光性能的影响.     

白光LED用MMoO_4∶Eu~(3+)红色荧光粉制备工艺研究

用溶胶-凝胶优化法合成了红色荧光粉MMoO4∶Eu3+(M=Ca、Sr、Ba),通过SEM、PL表征了荧光粉的形貌及发光性能。结果表明:烧结温度为800℃时,颗粒粒度分布均匀,粒径约为0.5-1μm,有很好的分散性;掺杂0.25molEu2O3在395nm和464nm两主激发峰下,均可得到616nm处红光发射极峰,属于Eu3+典型的5 D0→7F2的跃迁所致;助熔剂NH4F明显提高了钼酸盐荧光粉的发光强度;通过比较M0.5MoO4∶Eu03.+25,Li0+.25(M=Ca、Sr、Ba)发光性能得知:在395nm激发下,Ca0.5MoO4∶Eu30.+25,Li0+.25荧光粉最有利于提高发光强度。     

一种白色发光二极管用Ag2Sr(MoO4)2∶xSm3+红色荧光粉发光性能的研究

采用水热制备系列Ag2Sr(MoO4)2∶xSm3+红色荧光粉,并对其进行X射线衍射、扫描电镜和荧光光谱测试.结果 表明,Sm3+的掺入不影响Ag2 Sr(MoO4)2∶xSm3+晶相的形成,合成的荧光粉体晶粒较小,粒度分布均匀.在紫外灯照射下,Ag2 Sr(MoO4)2∶0.08Sm3+荧光粉发出更亮的红光,而且具有...     

溶胶-凝胶法合成LED用红色发光材料R2-xEux（MoO4）3（R=Gd，Y，La）及性能研究

采用溶胶-凝胶法合成了发光二极管（LED）用R2-xEux（MoO4）3（R=Gd，YLa；0≤x≤2）系列高亮度红色荧光粉，并对其结构与发光性能进行了详细研究。采用粉末x射线衍射（XRD）测量了不同温度下合成的样品结构变化情况，发现当R=y和Gd时，它们具有单斜和正交两种结构：当R=La时，荧光粉只有一种单斜结构．同时用荧光光谱对它们的发光性能进行了研究，发现在相同条件下（相同温度，相同时间，相同浓度）得到的样品的发光强度顺序为La0.8Eu1.2（MoO4）3〉Gd0.8Eu1.2（MoO4）3〉Y0.8Eu1.2（MoO4）3，且它们在395和465nm均有较强的有效激发，这两种波长正好与商用的GaN基LED芯片相匹配,同时研究了煅烧温度及掺杂浓度对其发光性能的影响。     

双钙钛矿结构固体氧化物燃料电池阴极SmBaFe_(2-x)Co_xO_(5+δ)的制备与性能研究

采用溶胶-凝胶法制得双钙钛矿钐钡铁钴氧化物[SmBaFe_(2-x)Co_xO_(5+δ)(x=0,0.5,1.0,1.5)]系列阴极材料,并对制得的SmBaFe_(2-x)Co_xO_(5+δ)进行了测试。研究结果表明:制得的SmBaFeCoO_(5+δ)形成了单一的钙钛矿结构,颗粒较小,分散较均匀,颗粒之间连接性好并拥有适当的孔隙率,与电解质结合较致密,在Co掺杂量x=1.0,850℃条件下,制得的SmBaFeCoO_(5+δ)的极化界面电阻(Rp)最小为0.763,电导率最大达到58.68S/cm,在固体氧化物燃料电池(SOFC)领域具有较好的应用前景。     

超细Mo-30Cu复合粉末的烧结行为

采用溶胶-喷雾干燥-煅烧-氧还原方法制备了晶粒尺寸为17-30 nm的超细Mo-30Cu复合粉末,在制备过程中经历了一系列的相转变,由喷雾干燥复合盐前驱体Cu7.6O8(NO3)+(NH4)2(Mo4O13)+(NH4)6(Mo7O24)(H2O)4+Cu4Mo5O17+CuMoO4在450℃煅烧后转变为CuMoO4+MoO3复合氧化物,在300℃低温还原转变为MoO2+Cu2O+Cu三相,再在700℃高温还原完全转变为Mo+Cu两相复合粉末.该粉末在1050-1200℃烧结时从亚稳态Mo(Cu)固溶体逐渐转变为Mo和Cu相,在1050℃烧结后得到致密度为99.7%的细晶合金.合金的最大抗拉强度可达755 MPa,最大延伸率可达15.8%.     

Li1.3Al0.3Ti1.7(PO4)3的溶胶-凝胶法制备及其性质研究

采用溶胶凝胶法及固相反应法合成锂离子固体电解质Li1.3Al0.3Ti1.7(PO4)3,用X射线衍射检测合成产物的物相,用循环伏安及交流阻抗技术测试产物的电化学窗口及离子电导率等电化学性质。研究表明溶胶凝胶法合成的Li1.3Al0.3Ti1.7(PO4)3的电化学窗口为2.4V。与固相反应法相比,溶胶凝胶法合成的Li1.3Al0.3Ti1.7(PO4)3具有更好的结晶性,其烧结片具有较高的离子电导率和较小的活化能。     

溶胶-凝胶法引入ZnO-2B2O3-7SiO2玻璃对BaO-Sm2O3-4TiO2陶瓷性能的影响

采用固相反应法合成BaO-Sm2O3-4TiO2 (BST)陶瓷粉体.系统研究了溶胶-凝胶法引入ZnO-2B2O3-7SiO2 (ZBS)玻璃对BST陶瓷烧结特性、物相组成、微观形貌及介电性能的影响.结果表明,添加ZBS玻璃的陶瓷试样主晶相仍为类钙铁矿钨青铜结构的BaSm2Ti4O12,次晶相为Sm2Ti2O7.通过溶胶-凝胶法添加6％(质量分数)的ZBS玻璃,可使BST陶瓷的烧结温度从1350℃降低到1050℃,在1050℃烧结3h所得BST陶瓷介电性能优良:εr=60.17,tanδ=0.004,τf=-7.9×10 6/℃.     

PMMA/SiO_2-TiO_2杂化纤维的制备与表征

以正硅酸乙酯和钛酸四丁酯为前驱体,乙烯基三乙氧基硅烷为偶联剂,采用溶胶凝胶原位聚合法制备了聚甲基丙烯酸甲酯/二氧化硅-二氧化钛(PMMA/SiO2-TiO2)杂化溶胶,陈化后用提拉法制得杂化纤维。研究了溶胶的杂化反应机理;使用红外光谱(IR)、扫描电子显微镜(SEM)、紫外-可见光谱(UV-Vis)、荧光光谱(FL)和热重分析(TGA)分析了杂化纤维的结构与性能。结果表明,PMMA与SiO2-TiO2之间通过化学键连接;纤维直径为150μm,在纤维内部有机无机相间形成均一的连续相;TiO2的引入增加了其抗紫外性;杂化纤维具有荧光性能;其耐热性能优于纯PMMA。     

VLE data for CO2-CF2Cl2, N2-CO2, N2-CF2Cl2 and N2-CO2-CF2Cl

Knowledge about vapour-liquid (VLE) is required as a basis of reliable calculations for separation processes. Correlations available for the prediction of T, p, x, y data are less accurate for mixtures at high pressures and mixtures containing supercritical components. The results of VLE experiments are reported and compared with data calculated with equations of state.     

Preparation of ZrO2-CeO2 and HfO2-CeO2 nanopowders

We prepared weakly agglomerated powders of ZrO₂-CeO₂ and HfO₂-CeO₂ solid solutions 5–8 nm in particle size, consisting of monoclinic and tetragonal phases. After heat treatment at 1200°C, the crystallite size was 30 and 14 nm, respectively. We also examined the effect of precipitate freeze drying on the crystallization of hafnia-based solid solutions containing up to 20 mol % CeO₂.     

Thermal diffusion in binary mixtures H2-CCl2F2 and H2-CHClF2

Thermal diffusion coefficients were measured in two gaseous mixtures, in which one component was close to the critical temperature, in the pressure range (19.6–127.4)·10⁴ N/m² and at a freon concentration of 0.25–0.8.     

Comparison of the Electronic Structures of La2CuO4, Sr2CuO2Cl2, and Sr2CuO2F2

First-principles cluster calculations are reported of the local electronic structure of the three compounds: La₂CuO₄, Sr₂CuO₂Cl₂, and Sr₂CuO₂F₂. The copper ${\text{3d}}_{x^2 - y^2 } $ and the planar oxygen 2p _σ atomic orbitals exhibit a similar degree of covalency. The out-of-plane orbitals, however, are quite different with the ${\text{3}}d_{3z^2 - r^2 } $ atomic orbital lowered significantly in energy for chlorine and fluorine apical positions.     

Radial GRIN glasses in Li2O-Na2O-Al2O3-TiO2-SiO2 systems

A series of GRIN glass rods have been developed in Li2O-Na2O-Al2O3-TiO2-SiO2 systems. Negative radial refractive index profiles were generated by exchanging Na+ for Li+ ions in these glass rods. It has been observed that TiO2 plays a vital role in increase in the profile depth and maximum change in the refractive index because of its ambivalent nature. Change in the refractive index can be further increased by increasing the concentration of exchanging cation in the base glass.     

Elastic and Electronic Properties of Superconducting CaPd 2 As 2 and SrPd 2 As 2 vs. Non-superconducting BaPd 2 As 2

The first-principles calculations were performed to predict the elastic and electronic properties of the superconducting ThCr₂Si₂-type phases CaPd₂As₂ and SrPd₂As₂ in comparison with the non-superconducting CeMg₂Si₂-type phase BaPd₂As₂. Besides, the same properties were compared for CeMg₂Si₂- and ThCr₂Si₂-type polymorphs of BaPd₂As₂. We found that all these phases are mechanically stable and belong to soft materials with low hardness. The near-Fermi region is formed by the valence states of the blocks [Pd₂As₂] with decisive contributions of Pd 4d states. The values of N(E _F) increase in the sequence: CaPd₂As₂ < SrPd₂As₂ < BaPd₂As₂, i.e. in the reverse sequence relative to the transition temperatures T _C. Thus, the change in T _C cannot be explained by the electronic factor, i.e. by the simple correlation T _C～N(E _F). Most likely the decrease in T _C in the sequence CaPd₂As₂ → SrPd₂As₂ and the absence of a superconducting transition in BaPd₂As₂ are related to the structural factors and the peculiarities of the electron–phonon coupling mechanism.     

Si_2N_2O-Al_2O_3-La_2O_3和Si_2N_2O-Al_2O_3-CaO系统的亚固相关系

本文给出了 Si_2N_2O-Al_2O_3-La_2O_3和 Si_2N_2O-Al_2O_3-CaO 系统的亚固相图。实验结果表明:在 Si_2N_2O-Al_2O_3-CaO 系统中有一个未知结构的新化合物 CaO·Si_2N_2O,在3CaO·Si_2N_2O 和3CaO·Al_2O_3两化合物之间形成连续立方固溶体。而 Si_2N_2O-Al_2O_3-La_2O_3系统中则没有发现新化合物。在两个系统的富 Si_2N_2O区,过量的 Si_2N_2O 与 La_2O_3和 CaO 分别反应形成 Si_3N_4与 La_(10)[SiO_4]_(?)N_2(H-相)(和 CaSiO_3。所研究的这两个三元系统中,分别形成了如下几个四元相容性区。在 Si_2N_2O-Al_2O_3-La_2O_3系统内有:H-Si_3N_4-La_2O_3·Si_2N_2O-La_2O_3·Al_2O_3;H-Si_3N_4-La_2O_3·Al_2O_3-La_2O_3·11 Al_2O_3;H-Si_3N_4-La_2O_3·11 Al_2O_3-Al_2O_3;H-Si_3N_4-Al_2O_3-O′s.s;H-Si_3N_4-O′s.s-Si_2N_2O在 Si_2N_2O-Al_2O_3-CaO 系统内有:Si_3N_4-CaSiO_3-CaO·Si_2N_2O-3CaO·Al_2O_3;Si_3N_3-CaSiO_3-3CaO·Al_2O_3-2CaO·Al_2O_3·SiO_(?);Si_(?)N_(?)-CaSiO_3-2CaO·Al_2O_3·SiO_2-Al_2O_3;Si_3N_4-CaSiO_3-Al_2O_(?)-O′s.s;Si_3N_4-CaSiO_3-O′s.s-Si_(?)N_(?)O