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首页> 外文期刊>Journal of magnetism and magnetic materials >Magnetic anisotropy and anisotropic magnetoresistance in strongly phase separated manganite thin films
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Magnetic anisotropy and anisotropic magnetoresistance in strongly phase separated manganite thin films

机译:强相分离锰矿薄膜中的磁各向异性和各向异性磁阻

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摘要

The present study reports the impact of magnetic anisotropy (MA) on magnetotransport properties such as the magnetic transitions, magnetic liquid behavior, glass transition and anisotropic magnetoresistance (AMR) in epitaxial film (thickness 42 nm) of strongly phase separated manganite La_(5/8-y)Pr_yCa_(3/8)MnO_3 (y ≈ 0.4). Angle dependent magnetization measurement confirms the out-of-plane magnetic anisotropy with the magnetic easy axes aligned in the plane of the film and the magnetic hard axis along the normal to the film plane. The more prominent divergence between the zero filed cooled (ZFC) and field cooled warming (FCW) and the stronger hysteresis between the field cooled cooling (FCC) and FCW magnetization for H‖ shows the weakening of the magnetic liquid along the magnetic hard axis. The peak at T_P ≈ 42 K in FCW magnetization, which characterizes the onset of spin freezing shifts down to T_P ≈ 18 K as the field direction is switched from the easy axes (H‖) to the hard axis (H⊥). The glass transition, which appears at T_g ≈ 28 K for H‖| disappears for H⊥. The easy axis magnetization (M_‖) appears to saturate around H~20 kOe, but the hard axis counterpart ( M_⊥) does not show such tendency even up to H=50 kOe. MA appears well above the ferromagnetic (FM) transition at T ≈ 170 K, which is nearly the same as the Neel temperature (T_N) of M_⊥-T. The temperature dependent resistivity measured at H= 10 kOe applied along the easy axis (ρ_‖ - T) and the hard axis (ρ_⊥ - T) shows insulator metal transition (IMT) at ≈ 106 K and ≈ 99 K in the cooling cycle, respectively. The large difference between ρ_⊥ - T and ρ_‖ - T during the cooling cycle and in the vicinity of IMT results in huge AMR of ≈ -142% and -115%. The observed properties have been explained in terms of the MA induced variation in the relative fraction of the coexisting magnetic phases.
机译:本研究报告了强相分离锰矿La_(5 /)在外延膜(厚度42 nm)中磁各向异性(MA)对磁传输特性的影响,如磁跃迁,磁液体行为,玻璃化转变和各向异性磁阻(AMR)。 8-y)Pr_yCa_(3/8)MnO_3(y≈0.4)。取决于角度的磁化强度测量证实了平面外磁各向异性,其中磁易轴在薄膜平面内对齐,而磁硬轴沿薄膜平面的法线对齐。零磁场冷却(ZFC)和磁场冷却升温(FCW)之间的差异更明显,并且磁场冷却(FCC)和FCW对H''的磁化强度之间的磁滞越强,表明磁液体沿磁硬轴减弱。当磁场方向从易轴(H'')切换到硬轴(H⊥)时,FCW磁化过程中T_P≈42 K处的峰值表征了自旋冻结的开始,向下移动到T_P≈18K。玻璃化转变,对于H′|出现在T_g≈28K。消失为H⊥。易轴磁化强度(M_‖)似乎在H〜20 kOe附近饱和,而硬轴对应物(M_⊥)甚至在H = 50 kOe时也没有这种趋势。 MA在T≈170 K时出现在铁磁(FM)转变的上方,这几乎与M_⊥-T的Neel温度(T_N)相同。沿易轴(ρ_‖-T)和硬轴(ρ_⊥-T)施加的H = 10 kOe时测得的与温度相关的电阻率显示出冷却循环中≈106 K和≈99 K时的绝缘体金属转变(IMT) , 分别。在冷却周期中以及在IMT附近,ρ_⊥-T和ρ_‖-T之间的较大差异导致≈-142%和-115%的巨大AMR。观察到的特性已根据MA诱导的共存磁相相对分数的变化进行了解释。

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    CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India,AcSIR at CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India;

    CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India;

    School of Basic and Applied Sciences, K. R. Mangalam University, Sohna Road, Gurgaon 123103, Haryana, India;

    CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India;

    CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India,AcSIR at CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India;

    CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India,AcSIR at CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India;

    CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India,AcSIR at CSIR-National Physical Laboratory, K. S. Krishnan Road, New Delhi 110012, India;

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  • 正文语种 eng
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  • 关键词

    Manganite Thin Film; Phase Separation; Magnetic Liquid; Magnetic Anisotropy; Anisotropic Magnetoresistance;

    机译:锰薄膜相分离;磁性液体磁各向异性各向异性磁阻;

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