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手性拓扑半金属中的可控轨道角动量单极子

Controllable orbital angular momentum monopoles in chiral topological semimetals.

作者信息

Yen Yun, Krieger Jonas A, Yao Mengyu, Robredo Iñigo, Manna Kaustuv, Yang Qun, McFarlane Emily C, Shekhar Chandra, Borrmann Horst, Stolz Samuel, Widmer Roland, Gröning Oliver, Strocov Vladimir N, Parkin Stuart S P, Felser Claudia, Vergniory Maia G, Schüler Michael, Schröter Niels B M

机构信息

Laboratory for Materials Simulations, Paul Scherrer Institute, Villigen, Switzerland.

École Polytechnique Fédérale de Lausanne (EPFL), Lausanne, Switzerland.

出版信息

Nat Phys. 2024;20(12):1912-1918. doi: 10.1038/s41567-024-02655-1. Epub 2024 Sep 30.

Abstract

The emerging field of orbitronics aims to generate and control orbital angular momentum for information processing. Chiral crystals are promising orbitronic materials because they have been predicted to host monopole-like orbital textures, where the orbital angular momentum aligns isotropically with the electron's crystal momentum. However, such monopoles have not yet been directly observed in chiral crystals. Here, we use circular dichroism in angle-resolved photoelectron spectroscopy to image orbital angular momentum monopoles in the chiral topological semimetals PtGa and PdGa. The spectra show a robust polar texture that rotates around the monopole as a function of photon energy. This is a direct consequence of the underlying magnetic orbital texture and can be understood from the interference of local atomic contributions. Moreover, we also demonstrate that the polarity of the monopoles can be controlled through the structural handedness of the host crystal by imaging orbital angular moment monopoles and antimonopoles in the two enantiomers of PdGa, respectively. Our results highlight the potential of chiral crystals for orbitronic device applications, and our methodology could enable the discovery of even more complicated nodal orbital angular momentum textures that could be exploited for orbitronics.

摘要

轨道电子学这一新兴领域旨在为信息处理生成并控制轨道角动量。手性晶体是很有前景的轨道电子学材料,因为据预测它们具有类似单极子的轨道纹理,其中轨道角动量与电子的晶体动量呈各向同性对齐。然而,这种单极子尚未在手性晶体中被直接观测到。在此,我们利用角分辨光电子能谱中的圆二色性来成像手性拓扑半金属PtGa和PdGa中的轨道角动量单极子。光谱显示出一种稳健的极性纹理,它作为光子能量的函数围绕单极子旋转。这是潜在磁轨道纹理的直接结果,并且可以从局部原子贡献的干涉来理解。此外,我们还通过分别成像PdGa两种对映体中的轨道角动量单极子和反单极子,证明了单极子的极性可以通过主体晶体的结构手性来控制。我们的结果突出了手性晶体在轨道电子学器件应用方面的潜力,并且我们的方法可能会促成发现更复杂的节点轨道角动量纹理,这些纹理可用于轨道电子学。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/1fbd/11631750/0dba00e0dcde/41567_2024_2655_Fig1_HTML.jpg

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