论文标题
费米弧的出现和在抗fiferromagnet中的新型磁分裂
Emergence of Fermi arcs and novel magnetic splitting in an antiferromagnet
论文作者
论文摘要
费米(Fermi)弧是固体中异国情调状态的特征,因为它们在动量空间中将费米表面的常规概念视为封闭的轮廓。费米(Fermi)弧首先是在丘比特(Cuprates)中发现的,并由伪库引起。 Weyl半学提供了另一种产生费米弧的方法,它通过打破了3D Dirac Semimetal的时间逆向对称性(TRS)或反转对称性,这可以导致与具有相反手性的Weyl节点成对的Weyl Semimetal。与Chern数量相关的批量 - 边界对应关系导致费米弧在边界上的出现。在这里,我们提供了实验证据,表明,由于新型的频带分裂效果,在抗铁磁(AFM)立方NDBI状态下,磁性分裂的孔和电子样弧形出现在Neel温度以下。尽管TRS被AFM阶折断,但倒置和非词性TR都保留在散装中,从而排除了Weyl semimetal的可能性。观察到的磁分裂是高度不寻常的,因为它创建了相对曲率的带,随着温度的变化并遵循抗磁磁性阶阶参数。这与先前报道的磁分割案例完全不同,例如传统的Zeeman和Rashba,该病例保留了频带的曲率。因此,我们的发现代表了一种新型的效率状态,该状态是在存在远程AFM秩序的情况下通过新型的磁带拆分而创建的,而现有理论思想不太容易解释。
The Fermi arcs are signatures of exotic states in solids because they defy conventional concept of Fermi surfaces as closed contours in momentum space. Fermi arcs were first discovered in cuprates, and caused by the pseudogap. Weyl semimetals provided another way to generate Fermi arcs by breaking either the time reversal symmetry (TRS) or inversion symmetry of a 3D Dirac semimetal, which can result in a Weyl semimetal with pairs of Weyl nodes that have opposite chirality. The bulk-boundary correspondence associated with the Chern number leads to the emergence of Fermi arcs on the boundary. Here, we present experimental evidence that pairs of magnetically split hole- and electron-like Fermi arcs emerge below the Neel temperature, in the antiferromagnetic (AFM) state of cubic NdBi due to a novel band splitting effect. Whereas TRS is broken by the AFM order, both inversion and nonsymmorphic TRS are preserved in the bulk, precluding the possibility of a Weyl semimetal. The observed magnetic splitting is highly unusual, as it creates bands of opposing curvature, that changes with temperature and follows the antiferromagnetic order parameter. This is completely different from previously reported cases of magnetic splittings such as traditional Zeeman and Rashba, where the curvature of the bands is preserved. Therefore, our finding represents a new Fermionic state created by new type of magnetic band splitting in the presence of a long-range AFM order that are not readily explained by existing theoretical ideas.