A位的Sm掺杂对La0.67Sr0.33MnO3体系磁电性质的影响

通过实验研究了La0.67-xSmxSr0.33MnO3(x=0.00,0.10,0.20,0.30)体系的M-T曲线、ESR曲线、红外光谱、拉曼光谱、ρ-T曲线和MR-T曲线. 实验结果表明:随着Sm掺杂的增加,体系从长程铁磁有序向自旋团簇玻璃态和反铁磁状态转变,Sm掺杂引起的磁结构变化和额外磁性耦合将导致CMR效应.     

A位的Gd掺杂对La0.7Sr0.3MnO3体系磁电性质的影响

通过实验研究了La0.7-xGdxSr0.3MnO3(x=0.00,0.10,0.15,0.20,0.30,0.40,0.50,0.60,0.70)体系的M-T曲线、M-H曲线、红外光谱、拉曼光谱、ρ-T曲线和MR-T曲线.实验结果表明:随着Gd掺杂的增加,体系从长程铁磁有序向自旋团簇玻璃态和反铁磁状态转变,高掺杂时的输运性质在其磁背景下发生异常.Gd掺杂引起的磁结构变化和额外的磁性耦合将导致庞磁电阻效应.     

Dy的高掺杂对La0.7Sr0.3MnO3体系磁电性质的影响

通过实验研究了La0.7-xDyxSr0.3MnO3(x=0.00,0.30,0.40,0.50,0.60,0.70)体系的M-T曲线,M-H曲线,ρ-T曲线和MR-T曲线. 实验结果表明:随着Dy掺杂的增加,体系从长程铁磁有序向自旋团簇玻璃态、反铁磁及亚铁磁状态转变. x=0.30样品的M-T曲线上在TN附近出现磁化强度尖峰,x=0.40时尖峰消失. 对x=0.50样品,ZFC的M-T曲线随温度增加出现一个谷,随后在TN处出现峰;而FC的M-T曲线在低温下呈现负磁矩. 对x=0.60和0.70样品,不论FC还是ZFC的M-T曲线都类似于x=0.50的ZFC的M-T曲线. 高掺杂时的输运性质在其磁背景下发生异常. 这些奇异现象用Nel的双格子模型并联合M-H回滞曲线给予很好地解释.     

La0.67Ba0.33MnO3薄膜的激光辐照效应研究

利用脉冲激光沉积技术在LaAlO3(00l)单晶衬底上制备了La0.67Ba0.33MnO3薄膜,研究了CO2激光辐照对La0.67Ba0.33MnO3薄膜的微结构和磁电性能的影响.结果表明,经激光辐照后,La0.67Ba0.33MnO3薄膜的结晶性增强,薄膜应变减小;薄膜表面形貌由"岛状"结构变为"平原"结构,且粗糙度大大降低;同时,薄膜的饱和磁化强度、铁磁居里温度、金属-绝缘态转变温度和磁电阻增大,而矫顽场和电阻率减小.根据对传统退火效应的分析和理论计算,认为激光辐照导致的表面微结构的变化以及薄膜的氧含量和均匀性的提高对La0.67Ba0.33MnO3薄膜的磁电性能的改善与优化密切相关.     

Mo低掺杂La_(0.67)Sr_(0.33)MnO_3的磁电特性及室温磁电阻增强(英文)

采用固相反应法成功制备了Mo低掺杂La0.67Sr0.33Mn1-xMoxOc(x=0,0.02)单相多晶样品,系统研究了样品的磁性、电输运特性和磁电阻效应.发现Mo低掺杂对La0.67Sr0.33MnO3 的居里温度影响很小,但在La0.67Sr0.33MnO3铁磁基态背景下诱导出团簇自旋玻璃态行为.在低温区(0.1相似文献   

La0.7-xGdxSr0.3MnO3体系中的相分离

采用固相反应法制备了样品La0.7-xGdxSr0.3MnO3(x=0.00,0.20,0.30,0.40,0.50).通过测量样品的M～T曲线,ESR曲线,研究了La0.7-xGdxSrO0.3MnO3,体系中的相分离现象及相分离与CMR之间关系.结果表明:当x=0.30,0.40时,在PM-FM相变区产生相分离,并且磁电阻MR得到增强.研究结果表明:La0.7-xGdx Sr0.3MnO3中的相分离与Gd在A位的占位情况紧密相关,磁电阻MR的增强是在外磁场作用下,铁磁区扩大顺磁区减小引起的.     

La0.67-xSmxSr0.33MnO3(0.40≤x≤0.60)体系的TCR研究

通过测量La0.67-xSmxSr0.33MnO3(x=0.40,0.50,0.60)体系的M～T曲线和ρ～T曲线,研究了La位Sm掺杂对体系电阻温度系数 (TCR)的影响.实验结果表明:Sm掺杂引起的电阻率曲线急剧变化,导致大的TCR出现;TCR在x=0.40时出现峰值,随Sm掺杂的增加,TCR值逐渐减小.体系出现大的TCR,来源于Sm掺杂引起的晶格畸变和额外磁性.     

A位的Sm掺杂对La0.67Sr0.33MnO3体系磁电性质的影响

通过实验研究了La067-xSmxSr033MnO3(x=000，010，020，030)体系的M_T曲线、ESR曲线、红外光谱、拉曼光谱、ρ_T曲线和MR_T曲线. 实验结果表明：随着Sm掺杂的增加，体系从长程铁磁有序向自旋团簇玻璃态和反铁磁状态转变，Sm掺杂引起的磁结构变化和额外磁性耦合将导致CMR效应. 关键词： 磁结构 输运行为 庞磁电阻效应     

稀土掺杂(Sm、Gd、Dy)对La0.7Sr0.3MnO3室温磁电阻效应的增强

用固相反应法制备了La0.7-xSmxSr0.3MnO3,La0.7-xGdxSr0.3MnO3和La0.7-xDyxSr0.3MnO3(x=0.00,0.10,0.20,0.30)系列样品.通过M～T曲线,ρ～T曲线,研究了用稀土离子替代La对La0.7Sr0.3MnO3居里温度Tc和磁电阻的影响.结果表明:稀土离子掺杂是改变钙钛矿锰氧化物居里温度和增强MR的有效途径;适量掺杂可以在室温附近产生大的磁电阻.     

La0.7-xDyxSr0.3MnO3中的相分离和输运行为

通过测量样品的M-T曲线、 M-H曲线、 ESR曲线、ρ-T曲线和MR-T曲线, 研究了Dy掺杂(0.0≤x≤0.30)对La0.7Sr0.3MnO3磁电性质的影响. 实验结果表明 在TC处所有样品都经历了顺磁到铁磁的转变; 当T＜TC时, 掺杂样品进入自旋团簇玻璃态, 低温时显示出反铁磁性; x=0.20时, 样品在TC以上温区发生相分离; Dy掺杂引起的磁结构变化将导致CMR效应.     

Prediction of thermomagnetic properties of La0.67Ca0.33MnO3 and La0.67Sr0.33MnO3

The dependence of magnetization on the variation of temperature for La_0.67Ca_0.33MnO₃ and La_0.67Sr_0.33MnO₃ perovskite-type ceramic materials under an external magnetic field was modelled. Application of phenomenological model was performed, showing a good agreement with the experimental data. Temperature dependence of change of both magnetic entropy and specific heat under magnetic field 0.05?T was predicted for La_0.67Ca_0.33MnO₃ and La_0.67Sr_0.33MnO₃. Predicted values of maximum magnetic entropy change, full-width at half-maximum, relative cooling power and maximum specific heat under 0.05 T were evaluated.     

Charge-carrier density collapse in La0.67Ca0.33MnO3and La0.67Sr0.33MnO3 epitaxial thin films

We measured the temperature dependence of the linear high field Hall resistivity of ( K) and ( K) thin films in the temperature range from 4 K up to 360 K in magnetic fields up to 20 T. At low temperatures we find a charge-carrier density of 1.3 and 1.4 holes per unit cell for the Ca- and Sr-doped compound, respectively. In this temperature range electron-magnon scattering contributes to the longitudinal resistivity. At the ferromagnetic transition temperature a dramatic drop in the number of charge-carriers n down to 0.6 holes per unit cell, accompanied by an increase in unit cell volume, is observed. Corrections of the Hall data due to a non saturated magnetic state will lead a more pronounced charge-carrier density collapse. Received 22 July 1999 and Received in final form 7 October 1999     

La0.67Sr0.33MnO3薄膜光响应特性研究

实验测量了在不同温度和电场下,超巨磁电阻CMR(colossal magnetoresistance)薄膜材料La_0.67Sr_0.33MnO₃(LSMO)的光响应特性.发现样品被激光照射后,具有光诱导电阻变化的特性.在温度小于居里点Tc时,电阻随温度升高而增大,在Tc以上时,电阻则随温度升高而减小.通过对样品的光脉冲响应和偏置电场的关系分析,可认为其光响应特性的机理与激光激励下引起的自旋系统变化有关.     

Interface induced exchange bias effect in La0.67Sr0.33MnO3/SrIrO3 multilayer

Epitaxial superlattices of ferromagnetic/paramagnetic La_0.67Sr_0.33MnO₃/SrIrO₃ materials have been prepared on SrTiO₃ (100) substrate using pulse laser deposition technique. An unexpected onset of interface magnetic interaction has been observed around 40 K. Interestingly, magnetic exchange bias effect has been observed in both field cooled and zero field cooled magnetization loops, however, the shifting of loop is opposite in both measurements. Exchange bias field vanishes as temperature increases to interface magnetic ordering temperature. Moreover, exchange bias field is found to decrease with increasing cooling field. We believe that tuning of magnetic exchange at interface during field cooling induces this evolution in nature of exchange bias field.     

Variation of thermoelectric power with crystallite size of La0.67Sr0.33MnO3 manganites

Thermoelectric power (TEP) studies of La_0.67Sr_0.33MnO₃ polycrystalline manganite material system having varying particle size have been undertaken. These materials were prepared by citrate based sol–gel route by sintering at four different temperatures and were later characterized by X-ray diffraction (XRD), scanning electron microscopy, electrical resistivity, AC susceptibility, etc., studies. The XRD data were analyzed by Rietveld refinement technique. Thermopower versus temperature plots are found to exhibit two peaks and an effort has been made to explain the significance of both of them. Finally, with a view to understand the conduction mechanism in these materials, TEP data in the low-temperature ferromagnetic metallic (T < T _P) regime were analyzed using electron–magnon scattering phenomenon, while that in the high-temperature insulating (T > T _P) region were analyzed by small polaron hopping model.     

Evidence of orbital reconstruction at interfaces in ultrathin La0.67Sr0.33MnO3 films

Linear dichroism (LD) in x-ray absorption, diffraction, transport, and magnetization measurements on thin La(0.7)Sr(0.3)MnO(3) films grown on different substrates, allow identification of a peculiar interface effect, related just to the presence of the interface. We report the LD signature of preferential 3d-e(g)(3z(2)-r(2)) occupation at the interface, suppressing the double exchange mechanism. This surface orbital reconstruction is opposite to that favored by residual strain and is independent of dipolar fields, the chemical nature of the substrate and the presence of capping layers.     

Transport and magnetic properties of La1.48Nd0.4Sr0.12CuO4/La0.67Sr0.33MnO3 bilayer

We have grown La_1.48Nd_0.4Sr_0.12CuO₄/La_0.67Sr_0.33MnO₃ (LNSCO/LSMO) bilayer structure on SrTiO₃ (0 0 1) substrate. Both temperature dependences of resistivity and magnetization curves show anomalies between 60 < T < 80 K, where a low-temperature orthorhombic (LTO) to low-temperature tetragonal (LTT) structural transition is observed in LNSCO bulk crystal. It is suggested that the formation of domains in LSMO layer can relax the strains caused by the LTO–LTT transition in LNSCO layer.     

Structure and magnetic properties of CrN thin films on La0.67Sr0.33MnO3

High crystalline quality CrN thin films have been grown on La_0.67Sr_0.33MnO₃ (LSMO) templates by molecular beam epitaxy. The structure and magnetic properties of CrN/LSMO heterojunctions are investigated combining with the experiments and the first-principles simulation. The Nėel temperature of the CrN/LSMO samples is found to be 281 K and the saturation magnetization of CrN/LSMO increases compared to that of LSMO templates. The magnetic property of CrN/LSMO heterostructures mainly comes from Cr atoms of (001) CrN and Mn atoms of (001) LSMO. The (001) LSMO induces and couples the spin of the CrN sublattice at CrN/LSMO interface.     

Cu掺杂La0.67Sr0.33CuxMn1-xO3薄膜的光诱导效应研究

分别采用溶胶-凝胶和射频磁控溅射的方法制备了La0.67Sr0.33CuxMn1-xO3(x=0.05, 0.10和0.15)系列块材和薄膜,研究了Cu部分替代对薄膜光诱导特性的影响.实验结果表明随着Cu掺杂量的增加,薄膜的金属-绝缘转变温度向低温方向移动,且导电性降低.在金属相激光作用诱导电阻增大.光致电阻相对变化极大值随着Cu含量的增加而增大,当x =0.15时,光致电阻相对变化极大值达到58.3%,分析可能是由激光辐照诱导电子束缚于CuO2链外的局域态和晶格效应共同作用的结果.