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Anomalous and topological Hall effects in epitaxial thin films of the noncollinear antiferromagnet Mn_3Sn

机译:非共线反铁磁体Mn_3Sn外延薄膜中的异常和拓扑霍尔效应

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Noncollinear antiferromagnets with a D0_19 (space group = 194, P6_3/mmc) hexagonal structure have garnered much attention for their potential applications in topological spintronics. Here, we report the deposition of continuous epitaxial thin films of such a material, Mn_3Sn, and characterize their crystal structure using a combination of x-ray diffraction and transmission electron microscopy. Growth of MnjSn films with both (0001) c-axis orientation and (4043) texture is achieved. In the latter case, the thin films exhibit a small uncompensated Mn moment in the basal plane, quantified via magnetometry and x-ray magnetic circular dichroism experiments. This cannot account for the large anomalous Hall effect simultaneously observed in these films, even at room temperature, with magnitude σ_(xy)(μ_0H =0T) = 21 Ω~(-1) cm~(-1) and coercive field μ_0H_c = 1.3 T. We attribute the origin of this anomalous Hall effect to momentum-space Berry curvature arising from the symmetry-breaking inverse triangular spin structure of Mn_3Sn. Upon cooling through the transition to a glassy ferromagnetic state at around 50 K, a peak in the Hall resistivity close to the coercive field emerges. This indicates the onset of a topological Hall effect contribution, arising from a nonzero scalar spin chirality that generates a real-space Berry phase. We demonstrate that the polarity of this topological Hall effect, and hence the chiral nature of the noncoplanar magnetic structure driving it, can be controlled using different field-cooling conditions.
机译:具有D0_19(空间组= 194,P6_3 / mmc)六边形结构的非共线反铁磁体因其在拓扑自旋电子学中的潜在应用而备受关注。在这里,我们报告了这种材料Mn_3Sn的连续外延薄膜的沉积,并结合X射线衍射和透射电子显微镜对它们的晶体结构进行了表征。实现了具有(0001)c轴取向和(4043)织构的MnjSn薄膜的生长。在后一种情况下,薄膜在基底平面上表现出小的未补偿的Mn矩,通过磁力测定法和X射线磁性圆二色性实验进行定量。即使在室温下,这也不能解释在这些膜中同时观察到的大的异常霍尔效应,其幅度为σ_(xy)(μ_0H= 0T)= 21Ω〜(-1)cm〜(-1)和矫顽场μ_0H_c= 1.3 T.我们将此异常霍尔效应的起源归因于由Mn_3Sn的对称破坏逆三角自旋结构引起的动量空间Berry曲率。通过在大约50 K处转变为玻璃态铁磁态而冷却后,会出现接近矫顽场的霍尔电阻率峰值。这表明拓扑霍尔效应的产生是由非零的标量自旋手性引起的,该标量自旋手性产生实际空间的Berry相。我们证明,可以使用不同的场冷却条件来控制这种拓扑霍尔效应的极性,从而可以驱动非共面磁性结构的手性。

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