The topological phases of two-dimensional time-reversal symmetric insulators are classified by a Z2 topological invariant. Usually, the invariant is introduced and calculated by exploiting the way time-reversal symmetry acts in reciprocal space, hence implicitly assuming periodicity and homogeneity. Here, we introduce two space-resolved Z2 topological markers that are able to probe the local topology of the ground-state electronic structure also in the case of inhomogeneous and finite systems. The first approach leads to a generalized local spin-Chern marker, that usually remains well-defined also when the perpendicular component of the spin, Sz, is not conserved. The second marker is solely based on time-reversal symmetry, hence being more general. We validate our markers on the Kane-Mele model both in periodic and open boundary conditions, also in the presence of disorder and including topological/trivial heterojunctions.
Theory of local Z2 topological markers for finite and periodic two-dimensional systems / Baù, Nicolas; Marrazzo, Antimo. - In: PHYSICAL REVIEW. B. - ISSN 2469-9950. - 110:5(2024), pp. 1-13. [10.1103/PhysRevB.110.054203]
Theory of local Z2 topological markers for finite and periodic two-dimensional systems
Marrazzo, Antimo
2024-01-01
Abstract
The topological phases of two-dimensional time-reversal symmetric insulators are classified by a Z2 topological invariant. Usually, the invariant is introduced and calculated by exploiting the way time-reversal symmetry acts in reciprocal space, hence implicitly assuming periodicity and homogeneity. Here, we introduce two space-resolved Z2 topological markers that are able to probe the local topology of the ground-state electronic structure also in the case of inhomogeneous and finite systems. The first approach leads to a generalized local spin-Chern marker, that usually remains well-defined also when the perpendicular component of the spin, Sz, is not conserved. The second marker is solely based on time-reversal symmetry, hence being more general. We validate our markers on the Kane-Mele model both in periodic and open boundary conditions, also in the presence of disorder and including topological/trivial heterojunctions.File | Dimensione | Formato | |
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