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钙钛矿型锰氧化物(La$lt;sub$gt;0.8$lt;/sub$gt;Eu$lt;sub$gt;0.2$lt;/sub$gt;)$lt;sub$gt;4/3$lt;/sub$gt;Sr$lt;sub$gt;5/3$lt;/sub$gt;Mn$lt;sub$gt;2$lt;/sub$gt;O$lt;sub$gt;7$lt;/sub$gt;的磁性和电性研究
引用本文:万素磊,何利民,向俊尤,王志国,邢茹,张雪峰,鲁毅,赵建军.钙钛矿型锰氧化物(La$lt;sub$gt;0.8$lt;/sub$gt;Eu$lt;sub$gt;0.2$lt;/sub$gt;)$lt;sub$gt;4/3$lt;/sub$gt;Sr$lt;sub$gt;5/3$lt;/sub$gt;Mn$lt;sub$gt;2$lt;/sub$gt;O$lt;sub$gt;7$lt;/sub$gt;的磁性和电性研究[J].物理学报,2014,63(23):237501-237501.
作者姓名:万素磊  何利民  向俊尤  王志国  邢茹  张雪峰  鲁毅  赵建军
作者单位:1. 内蒙古科技大学包头师范学院物理科学与技术学院, 包头 014030;2. 内蒙古科技大学, 内蒙古自治区白云鄂博矿多金属资源综合利用重点实验室, 包头 014010
摘    要:采用传统固相反应法制备钙钛矿型锰氧化物 (La0.8Eu0.2)4/3Sr5/3Mn2O7多晶样品, X-射线衍射分析表明, 样品(La0.8Eu0.2)4/3Sr5/3Mn2O7结构呈现良好的单相. 通过磁化强度随温度的变化曲线(M-T)、不同温度下磁化强度随磁场的变化曲线(M-H)和电子自旋共振谱发现: 在300 K以下, 随着温度的降低, 样品先后经历了二维短程铁磁有序转变 (TC2D ≈ 282 K)、三维长程铁磁有序转变(TC3D ≈ 259 K)、奈尔转变(TN ≈ 208K)和电荷有序转变(TCO ≈ 35 K); 样品 (La0.8Eu0.2)4/3Sr5/3Mn2O7TN以下, 主要处于反铁磁态; 在TC3D达到370 K时, 样品处于铁磁-顺磁共存态, 在370 K以上时样品进入顺磁态. 此外, 分析电阻率随温度的变化曲线(ρ-T)得到: 样品在金属-绝缘转变温度(TP ≈ 80 K)附近出现最大磁电阻值, 其位置远离TC3D, 表现出非本征磁电阻现象, 其磁电阻值约为61%. 在TCO以下, 电阻率出现明显增长, 这是由于温度下降使原本在高温部分巡游的eg电子开始自发局域化增强所致. 通过对 (La0.8Eu0.2)4/3Sr5/3Mn2O7ρ-T 曲线拟合, 发现样品在高温部分的导电方式基本遵循小极化子的导电方式. 关键词: 磁性 电性 金属-绝缘转变温度 电子自旋共振

关 键 词:磁性  电性  金属-绝缘转变温度  电子自旋共振
收稿时间:2014-04-22

Magnetic and transport properties of bilayered perovskite manganites (La0.8Eu0.2)4/3Sr5/3Mn2O7
Wan Su-Lei,He Li-Min,Xiang Jun-You,Wang Zhi-Guo,Xing Ru,Zhang Xue-Feng,Lu Yi,Zhao Jian-Jun.Magnetic and transport properties of bilayered perovskite manganites (La0.8Eu0.2)4/3Sr5/3Mn2O7[J].Acta Physica Sinica,2014,63(23):237501-237501.
Authors:Wan Su-Lei  He Li-Min  Xiang Jun-You  Wang Zhi-Guo  Xing Ru  Zhang Xue-Feng  Lu Yi  Zhao Jian-Jun
Abstract:Samples of (La0.8Eu0.2)4/3Sr5/3Mn2O7 were prepared by solid state reaction method. X-ray diffraction patterns indicated that the sample shows no any asymmetry and no any trace of secondary phase. The magnetization curve as a function of temperature (M-T), the magnetization versus magnetic field (M-H) at different temperatures, and the electron spin resonance spectrum have been detected. The magnetization measurement reveals that with lowing temperature, all of the samples undergo a complex magnetic transition. They transform from the two-dimensional short-range ferromagnetic order at TC2D ≈ 282 K, and enter the three-dimensional long-range ferromagnetic state at TC3D ≈ 259 K. Then they step into the antiferromagnetic state at TN ≈ 208 K and enter electric charge temperature order at TCO ≈ 35 K. The antimagnetic phase is found in the sample (La0.8Eu0.2)4/3Sr5/3Mn2O7below TN. When TC3D=370 K, the paramagnetic phase and antimagnetic phase co-exist. When TC3D is above 370 K, only paramagnetic phase exists in the sample. Besides, through electrical resistivity versus temperature curve ρ-T, the sample shows the maximum magnetization electrical resistivity when metal-insulator transition temperature is reached TP ≈ 80 K, TP being far from TC3D. And the transition shows the phenomenon of intrinsic magnetization electrical resistance, MR ≈ 61%. The resistance begins to increase below TCO. Because of the lowing temperature, the itinerant electron eg becomes increasingly spontaneously localized. One can see from the fitted ρ-T curves that (La0.8Eu0.2)4/3Sr5/3Mn2O7 in high temperature range is in accordance with the small polaron mode range hopping conduction.
Keywords: magnetic property electrical property metal-insulator transition electron spin resonance
Keywords:magnetic property  electrical property  metal-insulator transition  electron spin resonance
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