Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
Phys Rev Lett. 2014 Mar 21;112(11):117002. doi: 10.1103/PhysRevLett.112.117002. Epub 2014 Mar 20.
In mean-field descriptions of nodal d-wave superconductors, generic edges exhibit dispersionless Majorana fermion bands at zero energy. These states give rise to an extensive ground-state degeneracy, and are protected by time-reversal symmetry. We argue that the infinite density of states of these flat bands make them inherently unstable to interactions, and show that repulsive interactions lead to edge ferromagnetism which splits the flat bands. This edge ferromagnetism offers an explanation for the observation of the splitting of zero-bias peaks in edge tunneling in high-Tc cuprate superconductors. We argue that this mechanism for splitting is more likely than previously proposed scenarios and describe its experimental consequences.
在节线 d 波超导体的平均场描述中,一般的边缘在零能处表现出无弥散的马约拉纳费米子能带。这些状态导致了广泛的基态简并,并受到时间反演对称性的保护。我们认为,这些平带的无穷大态密度使它们本质上易受相互作用的影响,并表明排斥相互作用导致边缘铁磁性,从而分裂平带。这种边缘铁磁性为在高温超导 cuprate 边缘隧道中观察到零偏压峰的分裂提供了一种解释。我们认为,这种分裂机制比以前提出的方案更有可能,并描述了其实验后果。