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反铁磁体中由于磁分裂导致的费米弧的出现。

Emergence of Fermi arcs due to magnetic splitting in an antiferromagnet.

作者信息

Schrunk Benjamin, Kushnirenko Yevhen, Kuthanazhi Brinda, Ahn Junyeong, Wang Lin-Lin, O'Leary Evan, Lee Kyungchan, Eaton Andrew, Fedorov Alexander, Lou Rui, Voroshnin Vladimir, Clark Oliver J, Sánchez-Barriga Jaime, Bud'ko Sergey L, Slager Robert-Jan, Canfield Paul C, Kaminski Adam

机构信息

Ames Laboratory, Ames, Iowa, USA.

Department of Physics and Astronomy, Iowa State University, Ames, IA, USA.

出版信息

Nature. 2022 Mar;603(7902):610-615. doi: 10.1038/s41586-022-04412-x. Epub 2022 Mar 23.

Abstract

The Fermi surface plays an important role in controlling the electronic, transport and thermodynamic properties of materials. As the Fermi surface consists of closed contours in the momentum space for well-defined energy bands, disconnected sections known as Fermi arcs can be signatures of unusual electronic states, such as a pseudogap. Another way to obtain Fermi arcs is to break either the time-reversal symmetry or the inversion symmetry of a three-dimensional Dirac semimetal, which results in formation of pairs of Weyl nodes that have opposite chirality, and their projections are connected by Fermi arcs at the bulk boundary. Here, we present experimental evidence that pairs of hole- and electron-like Fermi arcs emerge below the Neel temperature (T) in the antiferromagnetic state of cubic NdBi due to a new magnetic splitting effect. The observed magnetic splitting is unusual, as it creates bands of opposing curvature, which change with temperature and follow the antiferromagnetic order parameter. This is different from previous theoretically considered and experimentally reported cases of magnetic splitting, such as traditional Zeeman and Rashba, in which the curvature of the bands is preserved. Therefore, our findings demonstrate a type of magnetic band splitting in the presence of a long-range antiferromagnetic order that is not readily explained by existing theoretical ideas.

摘要

费米面在控制材料的电子、输运和热力学性质方面起着重要作用。由于费米面在动量空间中由明确能带的闭合轮廓组成,被称为费米弧的不连续部分可能是异常电子态的特征,比如赝能隙。获得费米弧的另一种方法是打破三维狄拉克半金属的时间反演对称性或空间反演对称性,这会导致形成具有相反手性的外尔点对,并且它们在体能带边界处的投影由费米弧相连。在此,我们给出实验证据,表明在立方NdBi的反铁磁态中,由于一种新的磁分裂效应,类空穴和类电子费米弧对在尼尔温度(T)以下出现。观察到的磁分裂是不寻常的,因为它产生了具有相反曲率的能带,这些能带随温度变化并遵循反铁磁序参量。这与先前理论考虑和实验报道的磁分裂情况不同,比如传统的塞曼和 Rashba 效应,在这些效应中能带的曲率是保持不变的。因此,我们的发现展示了一种在长程反铁磁序存在下的磁能带分裂类型,现有理论观点难以对其进行解释。

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