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厚度与应变效应对La0.67Ca0.33MnO3薄膜电输运与居里温度的影响
引用本文:熊昌民,孙继荣,王登京,沈保根.厚度与应变效应对La0.67Ca0.33MnO3薄膜电输运与居里温度的影响[J].物理学报,2004,53(11):3909-3915.
作者姓名:熊昌民  孙继荣  王登京  沈保根
作者单位:中国科学院物理研究所与凝聚态物理中心磁学国家重点实验室,北京 100080
基金项目:国家自然科学基金(批准号:19934010)、国家杰出青年基金(批准号:50 225209)和国家重点基础研究发展规划项目资助的课题.
摘    要:在厚度为25—400nm范围内,系统地研究了 (001)SrTiO_3(STO), (001)LaAlO_3(LAO)衬底上La_0.67Ca_0.33Mn_O.3 (LCMO)薄膜的电输运与居里温度T_C随薄膜厚度及衬底的变化. 结果表明,随薄膜变薄,电阻率ρ增加,T_C降低. 对于同一薄膜厚度,LCMO/STO薄膜的ρ大于LCMO/LAO基上的薄膜的ρ. T_C衬底的依赖关系则与ρ相反. 分析表明,LCMO薄膜的低温区电阻温度(ρ-T) 符合关系式ρ=ρ_0+Bω_s/sin h^2(ω_s/2/k_BT)+CT^n, 其中ρ_0为剩余电阻;等号右端第二项反映软光学模声子对电子散射的贡献;第三项包括其余可能散射机 理在电输运过程中所起的作用;B,ωs(软光学模声子的平均频率)与C都为拟合系数. 高温区的电输运则由小极化子跃迁模型ρ=DT×exp(E_a/k_BT)描述(E_a为极化子激 发能). 根据ρ_0,ωs,E_a以及T_C变化,初步讨论了薄膜中的厚度与应变效应. 进一步 研究发现ωs,E_a的变化与T_C相关,从而说明极化子效应为影响T_C变化的主要因素. 关键词: 锰氧化物薄膜 电输运 居里温度 极化子

关 键 词:锰氧化物薄膜  电输运  居里温度  极化子
收稿时间:2004-01-17

Thickness and strain effects on electronic transport and Curie temperature in La_0.67Ca0.33MnO_3 films
Xiong Chang-Min,Sun Ji-Rong,Wang Deng-Jing and Shen Bao-Gen.Thickness and strain effects on electronic transport and Curie temperature in La_0.67Ca0.33MnO_3 films[J].Acta Physica Sinica,2004,53(11):3909-3915.
Authors:Xiong Chang-Min  Sun Ji-Rong  Wang Deng-Jing and Shen Bao-Gen
Abstract:La_0.67Ca_0.33Mn_O.3 films with thickness between 25 and 400nm were fabricated on (001)SrTiO_3 and (001)LaAlO_3 substrates, using pulsed laser deposition. The magnetization and resistivity ρ of the fil ms were studied as functions of thickness. The reduction of t causes the decrease of the Curie temperature T_C in addition to the increase of ρ of the films. Com pared with the compressive strain in the La_0.67Ca_0.33Mn_O.3/La AlO_3 films, the tensile strain in the La_0.67Ca_0.33Mn_O.3/SrTiO_3 films causes a faster reduction of T_C with t, and a larger value of ρ_0. The low_temperature ρ is found to follow well ρ=ρ_0+Bω_s/sin h^2(ω_s/2/k_BT)+CT^n, with ρ_0 being the residual resistivity. The second term arises fro m the scattering by a soft optical phonon mode, and the third term denotes the other possible transp ort mechanisms. B, ω_s(the frequency of a soft optical mode) and C are fitting parameters. At temperatures higher than T_C, ρ of all the films show activated conduction with ρ=DT×exp(E_a/k_BT). Here, E_a is the activation energy. Based on the investigation of ρ_0, ω_s and E_a, the thickness and strain effect s in the films are discussed, separately. Further study shows that the variation of T_C is mai nly associated with E_a and ω_s, confirming the crucial role of the electron_phonon coupling in the strain effects on T_C.
Keywords:manganite film  electronic transport  Curie temperature  polaron
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