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arXiv 2502.03751cond-mat.mtrl-scicond-mat.str-el
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非磁性 RuO$_2$ 中对称性破缺诱导的表面磁化

Symmetry-breaking induced surface magnetization in non-magnetic RuO$_2$

Dai Q. Ho, D. Quang To, Ruiqi Hu, Garnett W. Bryant, Anderson Janotti

AI总结:

本研究发现非磁性体态 RuO$_2$ 因局部对称性破缺在(110)表面产生自发磁化,引发自旋极化等光谱现象,揭示了表面磁结构的重要作用。

摘要:

交变磁性是一种新近被识别的磁性相,有别于铁磁性和反铁磁性。RuO$_2$ 被认为是典型的金属交变磁体,其临界温度高于室温。先前对 RuO$_2$ 异常磁性的解释依赖于理论预测,即由四重旋转对称性连接的两个 Ru 子晶格上的局域磁矩相当显著(约 1 $μ_B$),从而形成长程反铁磁序。然而,积累的实验数据表明,RuO$_2$ 中 Ru 上的局域磁矩微乎其微,表明该体态材料很可能是非磁性的。这一观察结果与 Ru 的 4$d$ 电子的离域性质以及金属态下的强屏蔽效应相一致。在本工作中,我们表明尽管体态非磁性,RuO$_2$(110) 表面却表现出自发磁化。我们将此效应归因于局部对称性破缺,这导致了电子重新分布和磁矩增强。表面磁性的出现引发了有趣的光谱现象,包括自旋极化表面态、自旋极化扫描探针显微图像,以及潜在的自旋相关输运效应。这些发现凸显了在原本非磁性的体态 RuO$_2$ 中表面磁结构的重要作用。

英文摘要:

Altermagnetism is a newly identified phase of magnetism distinct from ferromagnetism and antiferromagnetism. RuO$_2$ has been considered a prototypical metallic altermagnet with a critical temperature higher than room temperature. Previous interpretations of the unusual magnetic properties of RuO$_2$ relied on the theoretical prediction that local moments on two Ru sublattices, which are connected by four-fold rotational symmetry, are quite significant (approximately 1 $μ_B$), leading to long-range antiferromagnetic order. However, accumulated experimental data suggest that local moments on Ru in RuO$_2$ are vanishingly small, indicating that the bulk material is likely non-magnetic. This observation is consistent with the delocalized nature of the 4$d$ electrons of Ru and the strong screening effect in the metallic state. In this work, we show that despite the non-magnetic bulk, the RuO$_2$(110) surface exhibits spontaneous magnetization. We attribute this effect to the breaking of local symmetry, which results in electronic redistribution and magnetic moment enhancement. The emergence of surface magnetism gives rise to interesting spectroscopic phenomena, including spin-polarized surface states, spin-polarized scanning probe microscopy images, and potentially spin-dependent transport effects. These findings highlight the important role of surface magnetic structures in the otherwise non-magnetic bulk RuO$_2$.

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