Fe掺杂La0．8Sr0．2Co1-xFexO3磁性的研究

利用溶胶-凝胶法制备了一系列的La0.8Sr0.2Co1-xFexO3样品.通过研究在不同外加磁场下磁化强度和温度变化的关系发现,在较高的外场下La0.8Sr0.2Co1-xFexO3样品的磁性反转现象没有被观察到;在低场下La0.8Sr0.2Co1-xFexO3系统磁性反转现象被实现.这说明Fe的掺杂引起了La0.8Sr0.2Co1-xFexO3样品中铁磁和反铁磁之间的竞争,导致了La0.8Sr0.2Co1-xFexO3样品磁性反转;同时外加磁场的强弱影响了La0.8Sr0.2Co1-xFexO3系统磁性反转现象的发生,外加磁场增大使得在La0.8Sr0.2Co1-xFexO3样品中Co离子的自旋平行趋势更强,在铁磁和反铁磁之间的竞争中铁磁耦合占主导优势,因此在较高的外场下磁性反转现象没有被观察到.     

Co掺杂对钙钛矿锰氧化物La0.8Sr0.2MnO3磁性的影响

采用传统的高温固相反应法制备La0.8Sr0.2Mn1-xCoxO3（x=0,0.1）系列多晶样品,采用X射线衍射（XRD）测量样品的结构,并用物性测量系统（PPMS）探究样品的磁化强度随温度的变化曲线（M-T）,以及在不同的温度下磁化强度随外加磁场的变化曲线（M-H）。结果表明：当温度高于TG时,样品呈现出纯顺磁态,当TG相似文献   

稀土Pr掺杂纳米发光材料Sr_(0.2)Ca_(0.8)TiO_3的结构及光学性质

采用溶胶-凝胶法制备了Pr掺杂Sr0.2Ca0.8TiO3纳米粉体,用紫外可见光吸收光谱、X射线衍射、透射电镜进行结构表征,分析了不同温度下Sr0.2Ca0.8TiO3∶Pr的粒径大小以及结构变化,分析了其发光特性,并总结出最佳的合成温度为600℃.     

Gd3+对Ca0.8Zn0.2TiO3:Pr3+红色发光材料的敏化作用

采用溶胶-凝胶法在较低温度下合成了红色发光材料Ca0.8Zn0.2TiO3:0.002Pr3 ,xGd3 .金属离子预先溶解含有柠檬酸的乙二醇溶液中.XRD表明在800℃灼烧2h形成了钛酸盐的晶体.荧光检测结果表明所合成样品的特征激发峰为330nm、特征发射峰为614nm,分别对应于O(2p)→Ti(3d)带间跃迁和Pr3 的1D2→3H4的特征发射.样品的发光强度随x的不同而不同,发光强度增强了29%-69%.当x＝0.0005时,即nPr3 :nGd3 ＝4∶1时样品的红色发光强度最强,发光强度增强了69%.     

Oxygen transport properties of dense and porous (La0.8Sr0.2)0.99Co0.8Ni0.2O3-δ

We have determined k_ex and D_chem for (La_0.8Sr_0.2)_0.99Co_0.8Ni_0.2O_3-δ by the use of electrical conductivity relaxation on a dense sample and by applying the ALS model to measured AC impedance spectrum on a porous electrode. Extracting k_ex and D_chem from the methods resulted in comparable values. k_ex and D_chem also agreed well with literature values on La_0.8Sr_0.2CoO_3-δ, indicating that nickel substitution does not change the oxygen transport properties. k_ex of the porous sample was further found to decrease with a five times higher rate than D_chem when measured by using an Electrochemical Impedance Spectroscopy (EIS) over several days.     

溶胶-凝胶法制备的Ba0.8Sr0.2TiO3薄膜的结构及铁电性质研究

采用0.05mol/L的前驱体溶液,利用溶胶-凝胶法成功制备了室温下具有优良铁电性质的Ba_0.8Sr_0.2TiO₃ (BST)薄膜.X射线衍射分析表明,制得的BST薄膜室温下呈四方相,场发射扫描电子显微观测显示BST薄膜表面平整、致密、无裂纹出现,薄膜晶粒呈柱状结构、尺寸在150nm左右.电学测量表明制备的BST薄膜室温下具有优良的铁电性能.薄膜的剩余极化P_r约为35μC/cm²,矫顽电场E关键词：     

Mechanical properties of La0.58Sr0.4Co0.2Fe0.8O3-δ membranes

In this paper, we report on the mechanical properties of a La_0.58Sr_0.4Co_0.2Fe_0.8O_3-δ perovskite material. We use ring-on-ring bending tests with disk-shaped samples and depth-sensitive micro-indentation. In particular, the temperature dependency of fracture stress and elastic behavior are addressed. The fracture load is measured to be ～ 40% higher at room temperature (RT) than at 800 °C, which is due to the ferro-elasticity of material at RT. The stiffness shows an increase of about 50% above 600 °C and 700 °C in vacuum and air, respectively. The effect is attributed to a rhombohedral to cubic phase transition, which is not fully reversible upon cooling. The changes in phase composition with temperature are also confirmed by in-situ high temperature XRD. The transition appears to be associated with a change of heat capacity.     

不同制备方法合成的La0.9Sr0.1Ga0.8Mg0.2O3-δ材料晶体结构研究

分别用低温固相反应、高温固相反应和激光快速凝固技术(LRS)合成了固体氧化物燃料电池电解质材料La0.9Sr0.1Ga0.8Mg0.2O3-δ(LSGM),用Raman谱和X射线衍射研究了三组样品的晶体结构.三组样品Raman谱的明显差异表明它们分别属于三种不同的晶体结构.实验Raman谱与计算的三种可能晶体结构(立方...     

La1-xPrxCrO3纳米晶的结构和磁性质

我们用柠檬酸溶胶凝胶法成功制备了Pr掺杂La1-xPrxCrO3(x=0～0.6)纳米晶.在硝酸盐溶液中加入柠檬酸作为螯合剂,乙二醇为分散剂,得到干凝胶并在烧结温度为600 ℃时获得纯相钙钛矿结构纳米晶粉体,颗粒直径大约为40 nm且大小分布均匀.La0.5Pr0.5CrO3在场冷条件下的磁化强度以及在7K时的磁滞回线的测量结果表明,在260 K表现出顺磁到反铁磁转变,在200 K时磁化率达到最大值,随后磁化率随着温度的降低而急剧减小,在大约94 K的时候磁化率为0,随着温度的进一步降低,磁化率为负值.     

烧结温度、La掺杂对Bi_(1-x)La_xMnO_3结构及磁性能的影响

用溶胶-凝胶(so-lgel)法制备了多铁Bi1-xLaxMnO3(BLMO,0.1≤x≤0.4)系列样品.样品的结构表征(X-射线衍射,扫描电子显微镜)及差热-热重(TG-DTA)分析测量显示,形成稳定的BLMO钙钛矿相的烧结温度位于900~950℃.La掺杂对BLMO样品(950℃烧结)的结构和磁性能的影响也被仔细研究.结果显示,随着La掺杂减少,样品中BLMO钙钛矿相减弱,铁磁转变温度(TC)由53K降至41K,而饱和磁化强度经历了先降低再升高的变化.这可归因于La含量较少的样品中Bi空位浓度的增加诱导了Mn-O-Mn键角的减小和局域Mn4+离子的增多,使得Mn3+和Mn4+离子的铁磁超交换增强和Mn3+离子的dz2轨道有序受到局域破坏.     

La_(0.8-x)Ca_(0.2)MnO_3纳米颗粒的居里温度与磁热效应

采用溶胶 凝胶法制备了系列La0 .8-xCa0 .2 MnO3 多晶样品 ,用X射线衍射分析确定了样品的钙钛矿结构 ,用透射电子显微镜观察了样品的形貌及粒径分布情况 ,用PAR15 5型振动样品磁强计测量了样品的磁性随外场和温度的变化 ,确定样品的居里温度并计算了各样品的磁熵变 .磁测量及计算结果表明制备的各样品的居里温度在180— 2 6 0K的范围内且随焙烧温度和La3 离子空位浓度的不同而变化 ,不同温度焙烧的样品均有较大的磁熵变值 ,其中 110 0℃焙烧的La0 77Ca0 .2 MnO3,多晶样品在 2 40 5K ,H =1 0T的外场下的磁熵变达 3 76J/kg·K ,对实验结果做了定性的分析 .该材料具有较高的居里温度和较大的磁熵变 ,所需外场强度适中 ,电阻率高 ,性能稳定 ,适合做高温磁制冷材料 .     

Co掺杂对铁磁金属La0.8Sr0.2MnO3磁电阻影响机理

通过对La_0.8Sr_0.2Mn_1-yCo_yO₃(y≤02)饱和磁矩和输运的测量,研究了Co对La_0.8Sr_0.2MnO₃的磁电阻影响机制.结果表明,在La_0.8Sr_0.2Mn_1-yCo_yO₃（y≤02）中Co³⁺离子是低自旋态.由于Mn³⁺—O—Co³⁺—O—Mn³⁺类型的磁交换与Mn³⁺-Mn⁴⁺离子间双交换作用相比较弱,Curie温度T_C附近的磁电阻随着Co掺杂量的增加而降低.与此相反,由于Co²⁺离子与e_g巡游电子的反铁磁交换耦合作用,低温区间的磁电阻随着Co掺杂量的增加而升高. 关键词： 低自旋 磁电阻 磁交换作用     

零磁场下La_(0.67)Sr_(0.33-x)Na_xMnO_3的电输运特性研究

采用固相反应法制备了样品La0.67Sr0.33-xNaxMnO3(x=0.05,0.10,0.15,0.20,0.25,0.33).通过样品的红外吸收光谱、Ramam光谱、ρ～T曲线以及ρ～T拟合曲线,研究了样品的晶格结构变化和输运性质.结果表明:随Na掺杂的增加,Mn-O-Mn的键长、键角变化加大;体系属于双交换作用输运机制;在低温区(TTp),用[ρ-Texp(T0/T)]拟合得很好,ρ(T)符合极化子近邻跃迁模型.     

钴基掺杂氧化物结构特征的研究

利用溶胶-凝胶(sol-gel)法制备出了一系列La0.8Sr0.2Co1-xFexO3样品.xRD结果显示,在La0.8Sr0.2Co1-xFexO3系列样品中,未掺杂的La0.8Sr0.2CoO3样品具有很好的单相结构,并且衍射峰没有发生劈裂;而Fe掺杂的La0.8Sr0.2CoO3样品中几乎每个衍射峰都发生了劈裂,在Fe掺杂的La0.8Sr0.2CoO3样品中可能存在两种不同的晶体结构.利用xANES研究了La0.8Sr0.2Co1-xFexO3样品中Co离子和Fe离子的化合价发现,Fe离子存在两种不同的化合价态,即Fe3+和Fe4+离子,在La0.8Sr0.2Co1-xFexO3样品中形成了两个不同离子的富集区,一个是由Co3+、Co4+和Fe3+等离子组成的,一个是由Fe4+和Co3+、Co4+等离子组成的,因此在Fe掺杂的La0.8Sr0.2CoO3样品中存在两种不同的晶体结构.     

La_(0.5)Sm_(0.2)Sr_(0.3)MnO_3/Ag_x中的室温磁电阻增强

用固相反应法制备La0.5Sm0.2Sr0.3MnO3/(Ag2O)x/2(x=0.00,0.04,0.08,0.25,0.30)样品,通过M～T曲线,ρ～T曲线,ρ～T拟合曲线,研究样品的磁性质、输运行为、输运机制及磁电阻效应.结果表明:少量掺杂时Ag可能参与反应.掺杂量较多时,Ag主要以金属态分离到母体颗粒的界面处,使体系形成两相复合体.少量的Ag掺杂可以明显提高自旋相关散射产生的晶界磁电阻.掺Ag为30%摩尔比时,样品的电阻率较低掺杂样品的电阻率降低一个数量级,在300K、0.5T磁场下,磁电阻明显增强,达到9.4%,这与颗粒母体界面结构的改善有关,也与材料电阻率的降低有关.     

Effect of Terraces at the Interface on the Structural and Physical Properties of La_(0.8)Sr_(0.2)MnO_3 Thin Films

Employing atomic force microscopy,transmission electron microscopy and the second harmonic generation technique,we carefully explore the structural properties of 6-unit-cell-thick La_(0.8)Sr_(0.2)MnO_3 films grown on SrTiO_3 with atomically flat TiO_2-terminated terraces on the surface.The results clearly demonstrate that the terraces on the surface of TiO_2-terminated SrTiO_3 can improve the layer-by-layer epitaxial growth of the manganite films,which results in uniform film coverage at the beginning of growth and thus reduces the substrate-induced disorder at or near the interface.Comparing the magnetic and transport properties of La_(0.8)Sr_(0.2)MnO_3 films with the thicknesses varying from 6 unit cells to 80 unit cells grown respectively on as-received SrTiO_3 and TiO_2-terminated SrTiO_3,it is found that these atomically flat terraces on the surface of TiO_2-terminated SrTiO_3 can greatly enhance the Curie temperature and conductivities of the ultrathin La_(0.8)Sr_(0.2)MnO_3 films with thickness less than 50 unit cells,while no obvious difference is detected in the magnetic and transport properties of the 80unit-cell thick films.     

Current-dependent positive magnetoresistance in La_(0.8)Ba_(0.2)MnO_3 ultrathin films

We report an investigation into the magnetoresistance(MR) of La_(0.8) Ba_(0.2) Mn O_3 ultrathin films with various thicknesses. While the 13 nm-thick film shows the commonly reported negative magnetoresistive effect, the 6 nm-and 4 nmthick films display unconventional positive magnetoresistive(PMR) behavior under certain conditions. As well as the dependence on the film's thickness, it has been found that the electrical resistivity and the PMR effect of the thinner films are very dependent on the test current. For example, the magnetoresistive ratio of the 4 nm-thick film changes from +46%to-37% when the current is increased from 10 n A to 100 n A under 15 k Oe at 40 K. In addition, the two thinner films present opposite changes in electrical resistivity with respect to the test current, i.e., the electroresistive(ER) effect, at low temperatures. We discuss the complex magnetoresistive and ER behaviors by taking account of the weak contacts at grain boundaries between ferromagnetic metallic(FMM) grains. The PMR effect can be attributed to the breaking of the weak contacts due to the giant magnetostriction of the FMM grains under a magnetic field. Considering the competing effects of the conductive filament and local Joule self-heating at grain boundaries on the transport properties, the dissimilar ER effects in the two thinner films are also understandable. These experimental findings provide an additional approach for tuning the magnetoresistive effect in manganite films.     

二维周期性多孔La_(0.83)Sr_(0.17)Mn_(0.9)Zn_(0.1)O_3发射率研究

基于麦克斯韦方程组,利用时域有限差分方法(FDTD)计算了二维周期性多孔钙钛矿型氧化物La_(0.83)Sr_(0.17)Mn_(0.9)Zn_(0.1)O_3(LSMZO)的光谱特性,讨论了结构尺寸对光谱特性的影响。计算结果表明,当孔径约比热辐射波长小一个量级时,周期性多孔LSMZO的发射率比块体材料有所提高,这对改善热致变色材料的性能具有一定的指导意义。     

Mo掺杂La0.7Ca0.2Ba0.1Mn1-xMoxO3体系的磁电性质

本文采用固相反应法制备了高价态离子Mo掺杂的La0.7Ca0.2Ba0.1Mn1-xMoxO3(x=0,0.01,…,0.06)多晶样品,研究了Mo掺杂对样品的结构、磁性和磁电阻的影响.X射线衍射谱证实所有样品均为具有正交对称性的钙钛矿结构.零场冷却(ZFC)和加场冷却(FCH=0.01T)下其磁化～温度(M～T)曲线的测量表明样品随温度降低发生了从顺磁(PM)到铁磁(FM)的相变,T相似文献