La0.67Sr0.33MnO3中Ag-Ti的掺杂效应

将La0.67Sr0.33MnO3（LSMO）、Ag2O及TiO2粉混合经高温烧结后制备了钙钛矿相/xAg两相复合体系（x是Ag与钙钛矿材料的物质的量比）,系统地研究了Ag-Ti的共掺杂对LSMO电性和磁电阻效应的影响.0.07摩尔比Ti4＋离子的B位掺杂使LSMO的居里温度降至室温.Ag的掺入对Tc影响不大,Tp逐渐升高.由于钙钛矿颗粒属性的改善和金属导电通道的出现,材料的电阻率明显下降.Ag掺杂使室温磁电阻得到显著增强,室温下从x=0.30样品中得到最大的磁电阻,约为32%,是La0.67Sr0.33MnO3样品的8倍,La0.67Sr0.33Mn0.93Ti0.07O3样品的1.6倍.     

Co掺杂钙钛矿锰氧化物La0.8Sr0.2MnO3电磁特性研究

采用传统的高温固相反应法制备了La_0.8Sr_0.2Mn_1-xCo_xO₃(x = 0, 0.1, 0.3)多晶样品。系统研究了Co掺杂量对La_0.8Sr_0.2MnO₃(LSMO)多晶样品的类Griffiths相、磁熵变、临界行为和电输运性质的影响。研究结果表明: 制备的多晶样品均具有菱形对称结构; 三样品在低温磁转变温度(T_C2)以上均存在类Griffiths相; La_0.8Sr_0.2Mn_1-xCo_xO₃(x = 0, 0.1, 0.3)样品外加磁场为7 T的最大磁熵变ΔS_max分别为-2.28、-2.05和-2.75 J/(kg·K), Co元素的掺杂使得ΔS_max先减小后增大; 母相的临界行为与平均场模型拟合得最好, 掺杂后样品的临界行为和3D海森伯模型拟合最好; 母相为半导体材料, Co元素掺杂量达到0.1时在低温磁转变温度(T_C2)附近出现金属绝缘体转变; 高温区三样品的导电方式均满足小极化子模型。     

La0.7Ca0.3MnO3多晶样品中的相分离研究

采用固相反应法制备了La0.7Ca0.3MnO3多晶样品并借助X射线衍射,零场下的电阻测量以及电子顺磁共振技术对样品的结构、电子输运和磁性质进行了研究.实验结果表明,在居里温度TC附近,电子顺磁共振(ESR)谱线出现异常,谱线表现出明显的不对称,共振场随着温度的降低向低温方向移动.我们发现在居里温度TC以下用两个洛仑兹峰对ESR谱线可以进行较好的拟合,从而有力地证明了在相转变温度TC附近存在铁磁与顺磁相的共存.     

La0.7Sr0.3MnO3-Pb(Zr,Ti)O3双层膜中的磁电(ME)效应

由溶胶-凝胶法制备出锰酸盐La0.7Sr0.3MnO3粉料,经1300K热压并在1573K高温下烧结成块材,并与Pb(Zr,Ti)O3胶合形成弹性耦合双层膜.相较于涂敷膜(tape casting)复合样品,该双层膜显示出更为优良的ME耦合效应.横向耦合要比纵向耦合更为强烈,并当外加磁场为150 Oe时ME电压系数达到峰值.分析表明由磁场和频率变化导致的ME系数变化的实验值与理论值符合的很好.     

高能球磨法制备Nd0.7Sr0.3MnO3氧化物

经4h的高能球磨，钙钛矿结构氧化物Nd0.7Sr0.3Mn03完全合成，合成得到的样品颗粒尺寸范围在60～120nm，且大多数呈椭球状。继续球磨8h，出现了非晶无序相。然而，令人奇怪的是，再球磨非晶态样品6h，Nd0.7Sr0.3MnO3钙钛矿结构相又一次被合成。电子衍射结果也反应了初始原料随球磨时间的延长从多晶到非晶再到多晶的系列变化过程。     

La0.8-xNdxNa0.2MnO3的磁卡效应研究

用溶胶-凝胶法制备系列样品La0.8-xNdxNa0.2MnO3(x=0.00,0.05,0.10,0.15和0.20)钙钛矿锰氧化物.研究温度范围在240～340 K、外磁场0～1T下该系列样品的居里温度和磁熵变.发现样品的居里温度TC随x增加而减小,而且x=0.20、温度为295K时,最大磁熵变△SM为1.68 J/kg·K.实验结果表明钙钛矿锰氧化物La0.8-xNdxNa0.2MnO3有可能作为室温下的磁致冷材料的候选者.     

巡游铁磁体SrRuO3磁性的Preisach描述

测量了巡游铁磁体SrRuO3的零场冷却（ZFC）和加场冷却（FC）的磁化强度随温度的变化关系。以及不同温度下的磁滞回线，考虑了热涨落和自由能壁垒随温度的变化，改进了Preisach模型并对测量数据进行了拟合。数据模拟再现了测量结果的变化规律，包括在不同温度下的磁滞回线和在不同外磁场下的ZFC和FC磁化强度曲线等，对拟合出的巴克豪森跳跃谱进行了讨论。     

热处理对纳米钙钛矿氧化物La0.7Sr0.3FeO3—δ的电子结构的影响

利用ＰＥＧ法合成了粒度约为３０ｎｍ的处于正交结构的钙钛矿型氧化物Ｌａ０．７Ｓｒ０．３ＦｅＯ３－δ；通过对此氧化物进行高温后处理得到了立方和菱方结构的同化学计量比氧化物，测量了这三种不同结构样品的ＸＰＳ谱和Ｍｏｓｓｂａｕｅｒ谱，并同由固相反应法得到的同样化学计量的正交和立方混相氧化物进行了对比。结果表明Ｓｒ３ｄ由处于体相和表面两种状态组成，随粒度的增加，体相含量增加，同时Ｆｅ２ｐ３／２亦发生了明显的     

渠道火花烧蚀法制备La0.7Sr0.3MnO3薄膜

采用新型渠道火花烧蚀技术在LaAlO3(001)基片上生长了La0.7S0.3MnO3(LSMO)薄膜.X射线衍射对样品结构的分析表明,制备的LSMO薄膜具有c轴取向生长的特点,薄膜与基片间因晶格不匹配而受面内应力挤压,发生弛豫而出现两相.在室温下采用振动样品磁强计测试样品的面内方向磁滞回线,表明制备的LSMO样品具有软磁性,矫顽力Hc=13 Oe.通过标准四探针法测量了LSMO薄膜的室温薄膜电阻与外加磁场的关系,得知零场电阻率ρ(0)=19.4 mΩ·cm,室温下4800 Oe外场作用下的磁电阻变化率为2.25%,对此用双交换作用机制定性地加以了解释.     

La0.7Sr0.3FeO3-Sm0.2Ce0.8O2复合阴极制备及性能研究

采用固相反应法(SSR)和硝酸盐-甘氨酸燃烧法(GNP)合成La0.7Sr0.3FeO3(LSF)粉体,用于制备中温固体氧化物燃料电池的复合阴极LSF-Sm0.2Ce0.8O2(SDC).用交流阻抗谱研究复合阴极的组成、烧结温度、起始粉体性质等因素对电极界面比电阻的影响.结果表明,在LSF中加入适当比例的SDC可明显提高电极的性能.当SDC的加入量达到其渗流阀值(～50%,质量分数)时,在700℃复合阴极的界面比阻抗约为0.2 Ω·cm2,大约为纯LSF的十分之一.电极性能的明显提高的原因是电极离子电导率的提高、CeO2的本征催化性能以及电极三相线密度的增大.     

Magnetocaloric Effect in La0.7Cd0.3MnO3, La0.7Ba0.3MnO3, and Nd0.7Sr0.3MnO3

We have based on isothermal magnetization curves to study the magnetocaloric effect (MCE) in fine-grained perovskite manganites of La_0.7Cd_0.3MnO₃ (LCMO), La_0.7Ba_0.3MnO₃ (LBMO), and Nd_0.7Sr_0.3MnO₃ (NSMO) prepared by conventional solid-state reaction. Magnetic measurements were performed on a vibrating sample magnetometer, with a temperature increment of 1.0?K, and the applied field in the range of 0?C1.8?T. Under an applied field of 1.8?T, the maximum magnetic-entropy change obtained for LCMO, LBMO, and NSMO taking place at their Curie temperature are about 2.3, 2.1, and 5.1?J/(kg?K), respectively. The large entropy change in NSMO makes it suitable for magnetic-cooling applications.     

Low-field magnetoresistance in La0.7Sr0.3MnO3/BaTiO3 composites

A manganite composite series of (1 ? x)La_0.7Sr_0.3MnO₃/xBaTiO₃ (x = 0, 0.06, 0.12, and 0.18) has been fabricated by solid-state reaction combined with a high-energy mechanical milling method. Experimental results revealed that the insulator–metal transition temperature was shifted towards lower temperatures, and resistivity increases with increasing BaTiO₃ content in (1 ? x)La_0.7Sr_0.3MnO₃/xBaTiO₃. Meanwhile, the ferromagnetic–paramagnetic transition temperature was almost unchanged. The increase in magnetoresistance was observed in the all composites at whole measurement temperatures under an applied magnetic field of 3 kOe. Here, temperature dependences of magnetoresistance display a Curie–Weiss law-like behavior. The nature of this phenomenon is explained in detail.     

Tuning magnetic domain structure in nanoscale La0.7Sr0.3MnO3 islands

The realization of spin-based devices requires high density, ordered arrays of magnetic materials with a high degree of spin polarization at surfaces. We have synthesized, for the first time, highly spin polarized complex magnetic oxide nanostructures embedded in a paramagnetic matrix by electron beam lithography and ion implantation. Imaging the magnetic domains with X-ray photoemission electron microscopy and magnetic force microscopy reveals a delicate balance between magnetocrystalline, magnetoelastic, and magnetostatic energies that can be tuned by the choice of SrTiO3 substrate orientation, film thickness, island size, and island shape.     

Fabrication and Magnetic Properties of Electrospun La0.7Sr0.3MnO3 Nanostructures

La_0.7Sr_0.3MnO₃ (abbreviated as LSMO) nanostructures were fabricated by a simple electrospinning using a solution that contained poly(vinylpyrrolidone) (PVP), lanthanum, strontium and manganese nitrates. The LSMO nanostructures were successfully obtained from calcination of the as-spun LSMO/PVP composite nanofibers at 500–900 °C in air for 7 h. The as-spun and calcined LSMO/PVP composite nanofibers were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), and transmission electron microscopy (TEM). Analysis of phase composition by XRD revealed that all the calcined samples have a single rhombohedral LSMO phase. The SEM results showed that the crystal structure and morphology of the LSMO nanofibers were affected by the calcination temperature. Crystallite size of the nanoparticles contained in nanofibers increased with an increase in calcination temperature. The specific saturation magnetization (M _s ) values were obtained to be 1.23, 28.61, and 40.52 emu/g at 10 kOe for the LSMO samples calcined respectively at 500, 700, and 900 °C. It is found that the increase of the tendency of M _s is consistent with the enhancement of crystallinity, and the values of M _s for the calcined LSMO samples were observed to increase with increasing crystallite size. This increase in M _s for the calcined LSMO samples with increasing crystallite size may be explained by considering a magnetic domain of the samples.     

Ultrafast Orbital‐Oriented Control of Magnetization in Half‐Metallic La0.7Sr0.3MnO3 Films

Manipulating spins by ultrafast pulse laser provides a new avenue to switch the magnetization for spintronic applications. While the spin–orbit coupling is known to play a pivotal role in the ultrafast laser‐induced demagnetization, the effect of the anisotropic spin–orbit coupling on the transient magnetization remains an open issue. This study uncovers the role of anisotropic spin–orbit coupling in the spin dynamics in a half‐metallic La_0.7Sr_0.3MnO₃ film by ultrafast pump–probe technique. The magnetic order is found to be transiently enhanced or attenuated within the initial sub‐picosecond when the probe light is tuned to be s‐ or p‐polarized, respectively. The subsequent slow demagnetization amplitude follows the fourfold symmetry of the ${\mathrm{d}}_{x^2?y^2}$ orbitals as a function of the polarization angles of the probe light. A model based on the Elliott–Yafet spin‐flip scatterings is proposed to reveal that the transient magnetization enhancement is related to the spin‐mixed states arising from the anisotropic spin–orbit coupling. The findings provide new insights into the spin dynamics in magnetic systems with anisotropic spin–orbit coupling as well as perspectives for the ultrafast control of information process in spintronic devices.     

Exchange coupling and exchange bias in La0.7Sr0.3MnO3-SrRuO3 superlattices

La(0.7)Sr(0.3)MnO(3)-SrRuO(3) superlattices with and without nanometrically thin SrTiO(3), BaTiO(3) and Ba(0.7)Sr(0.3)TiO(3) interlayers were grown by pulsed laser deposition. Transmission electron microscopy studies showed coherent growth of La(0.7)Sr(0.3)MnO(3), SrRuO(3) and SrTiO(3) layers with atomically sharp interfaces, even if individual layers were as thin as one or two unit cells. In contrast, misfit dislocations and unit cell high interfacial steps were observed at the interfaces between BaTiO(3) and one of the ferromagnetic layers. The presence of the interlayers as well as these extended defects had a significant influence on the magnetic properties of the superlattices, especially on the antiferromagnetic interlayer exchange coupling between the La(0.7)Sr(0.3)MnO(3) and SrRuO(3) layers and the exchange biasing. Surprisingly, exchange biasing was found to increase with decreasing strength of the antiferromagnetic interlayer exchange coupling. This was explained by different magnetization reversal mechanisms acting in the regimes of strong and weak interlayer exchange coupling.