First-principles study of structural, electronic, and magnetic properties at the (0001)Cr2O3−(111)Pt interface

Marlies Reher, Nicola A. Spaldin, Sophie F. Weber
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引用次数: 0

Abstract

We perform first-principles density functional calculations to elucidate structural, electronic, and magnetic properties at the interface of (0001)Cr2O3(111)Pt bilayers. This investigation is motivated by the fact that, despite the promise of Cr2O3Pt heterostructures in a variety of antiferromagnetic spintronic applications, many key structural, electronic, and magnetic properties at the Cr2O3Pt interface are poorly understood. We first analyze all inequivalent lateral interface alignments to determine the lowest energy interfacial structure. For all lateral alignments including the lowest energy one, we observe an accumulation of electrons at the interface between Cr2O3 and Pt. We find an unexpected reversal of the magnetic moments of the interface Cr ions in the presence of Pt compared to surface Cr moments in vacuum-terminated (0001)Cr2O3. We also find that the heterostructure exhibits a magnetic proximity effect in the first three Pt layers at the interface with Cr2O3, providing a mechanism by which the anomalous Hall effect can occur in (0001)Cr2O3(111)Pt bilayers. Our results provide the basis for a more nuanced interpretation of magnetotransport experiments on (0001)Cr2O3(111)Pt bilayers and should inform future development of improved antiferromagnetic spintronic devices based on the Cr2O3Pt material system.

Abstract Image

(0001)Cr2O3-(111)Pt界面的结构、电子和磁性第一原理研究
我们进行了第一原理密度泛函计算,以阐明 (0001)Cr2O3-(111)Pt 双层膜界面的结构、电子和磁特性。尽管 Cr2O3-Pt 异质结构在各种反铁磁自旋电子应用中大有可为,但人们对 Cr2O3-Pt 界面的许多关键结构、电子和磁性能却知之甚少。我们首先分析了所有不等效的横向界面排列,以确定最低能量的界面结构。对于包括最低能量排列在内的所有横向排列,我们观察到电子在 Cr2O3 和 Pt 之间的界面聚集。我们发现,与真空端接 (0001)Cr2O3 中的表面 Cr 矩相比,铂存在时界面 Cr 离子的磁矩发生了意想不到的逆转。我们还发现,异质结构在与 Cr2O3 接口的前三层铂中表现出磁接近效应,这为 (0001)Cr2O3-(111)Pt 双层膜中出现反常霍尔效应提供了一种机制。我们的研究结果为更细致地解释 (0001)Cr2O3-(111)Pt 双层膜的磁传输实验提供了基础,并为未来开发基于 Cr2O3-Pt 材料体系的改进型反铁磁自旋电子器件提供了参考。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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CiteScore
8.60
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