2014
DOI: 10.1063/1.4878557
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Colossal anisotropic resistivity and oriented magnetic domains in strained La0.325Pr0.3Ca0.375MnO3 films

Abstract: Articles you may be interested inUltra-sharp oscillatory magneto-resistance in spatially confined La0.3Pr0.4Ca0.3MnO3 epitaxial thin films Appl. Phys. Lett. 105, 162409 (2014); 10.1063/1.4900491Three-dimensional strain state and spacer thickness-dependent properties of epitaxial Pr0.7Sr0.3MnO3/La0.5Ca0.5MnO3/Pr0.7Sr0.3MnO3 trilayer structure

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Cited by 11 publications
(4 citation statements)
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References 25 publications
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“…Here the doping ratio of Pr 3+ is selected as x = 0.3, so the content of Pr 3+ and La 3+ is approximately equal, which can result in much obvious EPS phenomenon [7]. Meanwhile, in order to only investigate the effect of the magnetic field on anisotropic transport behavior, the cubic STO single crystal with a lattice constant of a = 3.905 Å is chosen as the substrate, since it can provide an isotropic tensile stain on the LPCMO film [13,17]. Our results reveal that the magnetic field can induce a low resistance state which can be maintained after the removal of the magnetic field, showing a nonvolatile MR (defined by ΔR(H)/R(0) = [R(H) − R(0)]/R(0)) effect.…”
Section: Introductionmentioning
confidence: 99%
“…Here the doping ratio of Pr 3+ is selected as x = 0.3, so the content of Pr 3+ and La 3+ is approximately equal, which can result in much obvious EPS phenomenon [7]. Meanwhile, in order to only investigate the effect of the magnetic field on anisotropic transport behavior, the cubic STO single crystal with a lattice constant of a = 3.905 Å is chosen as the substrate, since it can provide an isotropic tensile stain on the LPCMO film [13,17]. Our results reveal that the magnetic field can induce a low resistance state which can be maintained after the removal of the magnetic field, showing a nonvolatile MR (defined by ΔR(H)/R(0) = [R(H) − R(0)]/R(0)) effect.…”
Section: Introductionmentioning
confidence: 99%
“…Jiang 等 [29] 研究了不同厚度 La 0.325 Pr 0.3 Ca 0.375 MnO 3 薄膜的磁性与电阻各向异性, 结果表明, 对于 30 nm 厚 的薄膜, 其各向异性电阻率(anisotropic resistivity, AR) 非常大(~10 5 %); 对于120 nm 厚的薄膜, 由于应变弛豫, 它的 AR 最大值显著降低(~2×10 3 %)。Nori 等 [30] 利用脉 冲激光沉积法在 Si(100)上制备了晶粒尺寸为 20~60 nm 的 La 0.7 Sr 0.3 MnO 3 薄膜, 并对其磁性能进行了表征。结 果表明, 晶粒致密排列的 La 0.7 Sr 0.3 MnO 3 薄膜居里温度 为 349 K, 而柱状晶粒组成的薄膜居里温度为 355 K, 这是目前已报道的沉积在 Si 衬底上 LSMO 薄膜最高的 居里温度。 最近, 人们对纳米结构的钙钛矿锰氧化物薄膜 的电磁输运特性亦进行了研究, 如 Hirooka 等 [31] 利 用原子力显微镜(AFM)辅助化学湿法刻蚀技术制备 了(La,Ba)MnO 3 纳米桥结构, 发现纳米桥的磁电阻 呈现 2 个数量级的变化。 近年来, Guo 等 [32] 采用 EBL 技术制备了不同宽度的 (La,Ca)MnO 3 薄膜微桥结 构, 电输运特性测量结果表明: 薄膜微桥宽度在 0.50 µm 以下, M-I 相变消失, 并且出现反常的正磁 电阻现象。…”
Section: 钙钛矿锰氧化物薄膜材料unclassified
“…The PS is characterized by the competition between the ferromagnetic metallic (FMM) phase and the antiferromagnetic insulating (AFI) phase in perovskite-structured manganites. 15 The transition, ranging from the AFI-dominant PS to the FMM-dominant PS in manganites, also named the melting transition under the high magnetic field condition, which were usually explored with microscopy techniques. 16,17 However, this electrical method is not applicable for the phase at nanometer scale due to the extremely strict measurement condition of the larger melting magnetic field for manganites.…”
Section: Introductionmentioning
confidence: 99%
“… 18–21 Although the electrical transport resistivity measurements can characterize the PS and AMR, it is inconvenient because they all have to make contacts to the sample. 15 Thus, a new method in the noncontact and nondestructive fashion is highly desired to probe the transport dynamics of the manganites.…”
Section: Introductionmentioning
confidence: 99%