论文标题
Fermi弧的栅极可调LIFSHITZ及其非本地运输特征的过渡
Gate-tunable Lifshitz transition of Fermi arcs and its nonlocal transport signatures
论文作者
论文摘要
Weyl半学的一个标志是在布里鲁因区域中Fermi Arcs(Fas)的出现,该区域连接了相反手性的投影的Weyl节点。未封闭的FA可以引起各种引起极大研究兴趣的异国情调。通常认为FAS的配置是由散装状态的带拓扑完全确定的,这似乎不可能操纵。在这里,我们表明可以简单地通过表面门电压来修改FAS。由于表面状态的渗透长度取决于平面内动量,因此表面栅极电压诱导有效的能量分散。结果,可以通过调谐表面栅极电压来实现表面带的连续变形。特别是,随着表面带的马鞍点符合费米的能量,拓扑Lifshitz转变发生在FAS中,在此期间,Weyl节点在此期间切换了由FAS连接的伴侣。因此,由FAS组成的磁性Weyl轨道在相反的表面和散装内部的手性Landau带上改变其构型。我们表明,可以通过磁场中的非局部传输测量值来探测这种效果,在该测量场中,表面栅极电压向非局部电导的开关打开和关闭了Lifshitz跃迁的信号。我们的工作开辟了一条新的途径,可以通过表面门操纵FAS,并探索与拓扑Lifshitz过渡相关的新型运输现象。
One hallmark of the Weyl semimetal is the emergence of Fermi arcs (FAs) in the surface Brillouin zone that connect the projected Weyl nodes of opposite chirality. The unclosed FAs can give rise to various exotic effects that have attracted tremendous research interest. The configurations of the FAs are usually thought to be determined fully by the band topology of the bulk states, which seems impossible to manipulate. Here, we show that the FAs can be simply modified by a surface gate voltage. Because the penetration length of the surface states depends on the in-plane momentum, a surface gate voltage induces an effective energy dispersion. As a result, a continuous deformation of the surface band can be implemented by tuning the surface gate voltage. In particular, as the saddle point of the surface band meets the Fermi energy, the topological Lifshitz transition takes place for the FAs, during which the Weyl nodes switch their partners connected by the FAs. Accordingly, the magnetic Weyl orbits composed of the FAs on opposite surfaces and chiral Landau bands inside the bulk change its configurations. We show that such an effect can be probed by the nonlocal transport measurements in a magnetic field, in which the switch on and off of the nonlocal conductance by the surface gate voltage signals the Lifshitz transition. Our work opens a new route for manipulating the FAs by surface gates and exploring novel transport phenomena associated with the topological Lifshitz transition.