Topological phase transition between a normal insulator and a topological metal state in a quasi-one-dimensional system

We theoretically report the finding of a new kind of topological phase transition between a normal insulator and a topological metal state where the closing-reopening of bandgap is accompanied by passing the Fermi level through an additional band. The resulting nontrivial topological metal phase is characterized by stable zero-energy localized edge states that exist within the full gapless bulk states. Such states living on a quasi-one-dimensional system with three sublattices per unit cell are protected by hidden inversion symmetry. While other required symmetries such as chiral, particle-hole, or full inversion symmetry are absent in the system.

Automated summary

A new kind of topological phase transition has been theoretically reported, where the closing-reopening of bandgap is accompanied by passing the Fermi level through an additional band. The resulting nontrivial topological metal phase is characterized by stable zero-energy localized edge states existing within the full gapless bulk states, protected by hidden inversion symmetry. Other required symmetries such as chiral, particle-hole, or full inversion symmetry are absent in the system.