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La0.67Sr0.08Na0.25MnO3的奇特输运性质及CMR效应
引用本文:彭振生,唐永刚,严国清,郭焕银,毛 强.La0.67Sr0.08Na0.25MnO3的奇特输运性质及CMR效应[J].物理学报,2007,56(3):1707-1712.
作者姓名:彭振生  唐永刚  严国清  郭焕银  毛 强
作者单位:(1)宿州学院巨磁材料研究室,宿州 234000; (2)宿州学院巨磁材料研究室,宿州 234000;中国科学技术大学结构分析重点实验室,合肥 230026
基金项目:国家自然科学基金重点项目(批准号:19934003)安徽省教育厅自然科学研究计划项目(批准号:2004KJ331),安徽省高等学校自然科学研究项目(批准号:2005KJ234,2006KJ266B),宿州学院教授(博士)科研启动基金(批准号:2006JB02)资助的课题.
摘    要:用固相反应法制备了La0.67Sr0.08Na0.25MnO3样品.通过磁化强度-温度(M-T)曲线、电阻率-温度(ρ-T)曲线以及ρ-T拟合曲线研究了样品的输运性质及庞磁电阻(colossal magnetoresistance,CMR)效应.结果表明,ρ-T曲线和磁电阻-温度(MR-T)曲线均出现双峰现象;高温峰是伴随顺磁-铁磁(PM-FM)相变出现绝缘体-金属(I-M)相变,低温峰是颗粒界面效应;两个绝缘相输运机理不同:较低温度下(248K<T<274K),ρ(T)符合极化子的可变程跃迁模型,而在更高温区(330K<T<374K),ρ(T)符合极化子近邻跃迁模型;两个类金属相输运机理也不同:在低温区(67K<T<186K),满足ρ-T2.5关系,输运机理是自旋波散射和电-磁子散射作用,而在高温区(292K<T<304K),满足ρ-T2关系,输运机理是单磁子散射作用. 关键词: 庞磁电阻 金属-绝缘体转变 晶界效应 输运行为

关 键 词:庞磁电阻  金属-绝缘体转变  晶界效应  输运行为
文章编号:1000-3290/2007/56(03)/1707-06
收稿时间:2006-07-12
修稿时间:07 12 2006 12:00AM

Peculiar transport properties and CMR effect of La0.67Sr0.08Na0.25MnO3
Peng Zhen-Sheng,Tang Yong-Gang,Yan Guo-Qing,Guo Huan-Yin and Mao Qiang.Peculiar transport properties and CMR effect of La0.67Sr0.08Na0.25MnO3[J].Acta Physica Sinica,2007,56(3):1707-1712.
Authors:Peng Zhen-Sheng  Tang Yong-Gang  Yan Guo-Qing  Guo Huan-Yin and Mao Qiang
Institution:1. CMR Materials Research Laboratory , Suzhou College , Suzhou 234000, China; 2. Structure Research Laboratary , University of Science and Technology of China , Hefei 230026, China
Abstract:The La0.67Sr0.08Na0.25MnO3 sample was prepared by solid-state reaction. The transport properties and CMR effect of the sample were studied through M-T curves, ρ-T curves and ρ-T fitted curves. The results show that: Both the ρ-T curves and the MR-T curve exhibit the double-peak phenomenon; the high-temperature peak corresponds to the I-M transition accompanied by the PM-FM transition, and the low-temperature peak is attributed to grain boundary effect. The two insulator phases have different transport mechanisms: in the low temperature range(248 K<T<274 K),ρ(T) accords with variable-range-hopping model of polaron, while in the high temperature range(330 K<T<374 K),ρ(T) accords with near- neighbor- hopping model of polaron; and the two metal-like phases also have different transport mechanisms: in the low temperature range(67 K<T<186 K), ρ(T) accords with the ρ-T2.5 relation, and the transport mechanism is the actions of spin wave scattering and electron-magneton scattering, while in the high temperature range(292 K<T<304 K),ρ(T) accords with the ρ-T2 relation, and the transport mechanism is single magneton scattering.
Keywords:colossal magnetoresistance  metal-insulator transition  grain boundary effect  transport behavior
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