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四方相 La(2/3)Ca(1/3)MnO3 薄膜中各向异性磁电阻和平面霍尔效应的现象学研究

A phenomenological approach to the anisotropic magnetoresistance and planar Hall effect in tetragonal La(2/3)Ca(1/3)MnO3 thin films.

机构信息

National Laboratory for Superconductivity, Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China.

出版信息

J Phys Condens Matter. 2010 Apr 14;22(14):146006. doi: 10.1088/0953-8984/22/14/146006. Epub 2010 Mar 23.

DOI:10.1088/0953-8984/22/14/146006
PMID:21389540
Abstract

A La(2/3)Ca(1/3)MnO(3) Hall bar with its long dimension roughly along the hard axis [110] was fabricated on a single-crystal-like tensilely strained film on SrTiO(3)(001). The anisotropic magnetoresistance (AMR) and planar Hall effect (PHE) have been studied at various external magnetic fields and temperatures. A phenomenological model in the high field limit is developed, and the galvanomagnetic tensor based on a tetragonal symmetry 4/mmm (D(4h)), applicable to epitaxial films on a substrate, has been obtained by expanding the tensor to the sixth order. The derived in-plane transverse resistance R(xy) shows a sin2φ(M) angular dependence, while the longitudinal R(xx) is constituted by not only a two-fold cos2φ(M) term, but also a four-fold cos4φ(M) term due to the square symmetry of the lattice. The model is in good agreement with the experimental results in high fields, while deviations are observed near the {100} easy axis with the decreasing field. Close inspection of the fitting parameters reveals the evolution of these term weights with temperature and magnetic field, which is distinct from conventional ferromagnetic metals and cannot be explained by the phenomenological model. An alternative mechanism for AMR, stemming from the magnetization-induced local orbit deformation through spin-orbit interaction, as previously proposed by O'Donnell et al, may be prevalent in manganites and other systems of complicated crystal structure.

摘要

在 SrTiO3(001) 上的单晶类拉伸应变膜上制备了一个长尺寸大致沿硬轴 [110] 的 La(2/3)Ca(1/3)MnO3 霍尔条。在不同的外磁场和温度下研究了各向异性磁电阻 (AMR) 和平面霍尔效应 (PHE)。在高场极限下开发了一个唯象模型,并通过将张量展开到第六阶,获得了适用于基底上外延膜的基于四方对称 4/mmm(D4h) 的旋磁张量。推导得出的面内横向电阻 R(xy) 表现出 sin2φ(M) 的角依赖性,而纵向电阻 R(xx) 不仅由两倍的 cos2φ(M) 项组成,而且由于晶格的正方形对称,还由四倍的 cos4φ(M) 项组成。该模型与高场下的实验结果吻合良好,而在磁场减小的情况下,在 {100} 易轴附近观察到偏差。对拟合参数的仔细检查揭示了这些项权重随温度和磁场的演变,这与传统的铁磁金属不同,不能用唯象模型来解释。一种替代 AMR 的机制,源于自旋轨道相互作用引起的磁化诱导局部轨道变形,正如 O'Donnell 等人之前提出的,可能在锰氧化物和其他复杂晶体结构的系统中普遍存在。

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