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Electric transport properties and temperature stability of magnetoresistance of composite system between La_(8/9)Sr_(1/45)Na_(4/45)MnO_3 and Sb_2O_3 被引量:4
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作者 Gui-Ying Wang Yong-Gang Tang +2 位作者 Qi-Xiang Song Ming-Yu Zhang Zhen-Sheng Peng 《Rare Metals》 SCIE EI CAS CSCD 2013年第4期363-368,共6页
The samples ofLa8/9Sr1/45Na4/45MnO3 (LSNMO)/x/2(Sb2O3) were prepared by the solid-state reaction method. The electric transport properties and the temperature stabil-ity of magnetoresistance (MR) of the samples ... The samples ofLa8/9Sr1/45Na4/45MnO3 (LSNMO)/x/2(Sb2O3) were prepared by the solid-state reaction method. The electric transport properties and the temperature stabil-ity of magnetoresistance (MR) of the samples were studied through the measurements of X-ray diffraction patterns, resistivity-temperature (ρ-T) curves, mass magnetization-temperature (σ-T) curves, and magnetoresistance-temper-ature (MR-T) curves. The results indicate that the p-Tcurves of the original material LSNMO show two peaks, and the phenomenon of two peaks of ρ-T curves disappears for the composite samples, which can be explained by a competition between surface-phase resistivity induced by boundary-dependent scattering and body-phase resistivity induced by paramagnetism-ferromagnetism transition. For all the sam-ples in the low temperature range, MR increases continu-ously with the decrease of temperature, which shows a characteristic of low-field magnetoresistance. However, MR basically keeps the same in the high temperature range. The paramagnetism-ferromagnetism transition is observed in the high temperature range due to a composite between perov-skite manganite and insulator, which can enhance the tem-perature of MR appearance in the high temperature range and make it to appear near room temperature. For the sample with x = 0.12, MR remains constant at the value of 7.5 % in the temperature range of 300-260 K, which achieves a tem-perature stability of MR near room temperature. In addition,for the sample with x = 0.16, MR is above 6.8 % in the high temperature range of 318-252 K (△T = 66 K). MR almost remains constant in this temperature range, which favors the practical application of MR. 展开更多
关键词 Electric transport property Temperaturestability of magnetoresistance Two-phase composite Perovskite manganite
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Transport properties and magnetoresistance in La_(0.8)Te_(0.2)MnO_3/ZrO_2 composites
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作者 王建元 翟薇 +1 位作者 金克新 陈长乐 《Chinese Physics B》 SCIE EI CAS CSCD 2011年第9期361-364,共4页
The transport properties and magnetoresistance of electron-doped manganate / insulator composites (Lao.sTeo.2MnO3)l-x/(ZrO2)x (x = 0, 0.3, and 0.5) are investigated. It is found that the metal-insulator transiti... The transport properties and magnetoresistance of electron-doped manganate / insulator composites (Lao.sTeo.2MnO3)l-x/(ZrO2)x (x = 0, 0.3, and 0.5) are investigated. It is found that the metal-insulator transition temperature of this system shifts to a lower value as the ZrO2 content increases. The introduction of ZrO2 enhances both the domain scattering and electron relative scattering in the metal transport region. In the adiabatic small polaron hopping transport region, the thermal activation energy seems invariable regardless of the ZrO2 content. The applica- tion of a magnetic field promotes the charge transportation capabilities of the composites, and the magnetoresistance is enhanced with an increase of the ZrO2 content. This could be attributed to the more remarkable modification effect of magnetic field on ordering degree in the composites than in pure Lao.sTe0.2MnO3. 展开更多
关键词 manganate composite transport property magnetoresistance
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(1-x)La_(0.6)Dy_(0.1)Sr_(0.3)MnO_3/(x/2)(Sb_2O_3)复合体系磁电阻及其温度稳定性
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作者 蔡之让 杨杰 +2 位作者 严国清 张明玉 宋启祥 《磁性材料及器件》 北大核心 2013年第2期5-8,68,共5页
用固相反应法制备了纯La0.6Dy0.1Sr0.3MnO3和(1-x)La0.6Dy0.1Sr0.3MnO3/(x/2)(Sb2O3)样品,研究了样品的电输运性质及高温磁电阻温度稳定性。结果表明,零场下,纯La0.6Dy0.1Sr0.3MnO3的ρ-T曲线出现双峰现象,高温峰是本征峰,较低温出现&qu... 用固相反应法制备了纯La0.6Dy0.1Sr0.3MnO3和(1-x)La0.6Dy0.1Sr0.3MnO3/(x/2)(Sb2O3)样品,研究了样品的电输运性质及高温磁电阻温度稳定性。结果表明,零场下,纯La0.6Dy0.1Sr0.3MnO3的ρ-T曲线出现双峰现象,高温峰是本征峰,较低温出现"肩峰"是非本征峰,复合体系在较低温的"肩峰"消失,用晶界效应予以解释;样品的电输运机制是,母体La0.6Dy0.1Sr0.3MnO3用ρ=ρ0+AT2拟合比较合理,复合样品用ρ=ρ0+AT2.5拟合比较合理;复合样品的MR-T曲线在高温出现一个平台,本征与非本征磁电阻的竞争结果是在高温区出现磁电阻平台,实现了高温区磁电阻的温度稳定性。 展开更多
关键词 钙钛矿锰氧化物 两相复合体 电输运性质 磁电阻 温度稳定性
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CuO复合对La_(0.80)Sr_(0.05)K_(0.15)MnO_3电输运和磁电阻的影响 被引量:4
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作者 王闻琦 王桂英 +3 位作者 唐永刚 毛强 刘鹏 彭振生 《稀土》 EI CAS CSCD 北大核心 2013年第3期64-68,共5页
用固相反应法制备了(1-x)La0.80Sr0.05K0.15MnO3/xCuO(x=0.00,0.04,0.08,0.10,0.20,0.30)二相复合体。通过X射线衍射图谱、扫描电子显微镜照片检测结构,表明形成完好的钙钛矿相和CuO相,CuO分布在钙钛矿颗粒之间,形成对钙钛颗粒的包覆。... 用固相反应法制备了(1-x)La0.80Sr0.05K0.15MnO3/xCuO(x=0.00,0.04,0.08,0.10,0.20,0.30)二相复合体。通过X射线衍射图谱、扫描电子显微镜照片检测结构,表明形成完好的钙钛矿相和CuO相,CuO分布在钙钛矿颗粒之间,形成对钙钛颗粒的包覆。通过测量零场和加场下的电阻率-温度曲线以及磁电阻-温度曲线,研究电输运性质及磁电阻效应,结果表明,CuO复合对La0.80Sr0.05K0.15MnO3电输运和磁电阻效应影响很大。在高温区出现磁电阻峰,表现出本征磁电阻特征,在低温区随温度降低磁电阻持续增大,表现出由界面引起的隧穿磁电阻特征,总的磁电阻是本征磁电阻与隧穿磁电阻的迭加,在中间温区出现磁电阻的温度稳定性。 展开更多
关键词 钙钛矿锰氧化物 CUO 二相复合体 电输运性质 磁电阻
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