Topological defect-mediated corner states and higher-order bulk topology in a two-dimensional crystalline insulator

TL;DR

This paper demonstrates the emergence of zero energy corner modes in a 2D topological insulator with higher-order topology, achieved through an unconventional stacking of 1D chains and tuning hopping parameters.

Contribution

It introduces a novel 2D crystalline topological insulator model exhibiting multiple second order topological phases with distinct corner modes, linked via bulk-corner correspondence.

Findings

Identification of multiple non-trivial second order topological phases.

Observation of zero energy corner modes on trimers and isolated sites.

Establishment of bulk-corner correspondence using winding numbers.

Abstract

We report appearance of non-trivial zero energy corner modes in the form of topological defects (trimers) in a carefully designed 2D crystalline topological insulator. The proposed scenario is developed via an unconventional stacking of 1D topological atomic chains with crystalline mirror symmetry along the diagonal (y=x) line. Our analysis shows that by systematically varying the hopping parameters t (intra-chain), v (within the unit cell) and w (between the unit cells) the system exhibits more than one distinct non-trivial second order topological phases. These phases are distinguished by the zero energy corner modes. In one of these phases the system supports four zero modes. Two of them reside on the trimers and the rest on isolated sites situated at the corner along the diagonal line. However, in the second case, the zero modes on the isolated sites persist at the corners while the zero modes on the trimers vanish. A critical look at the phase evolution of the Bloch states helps in investigating the topology of these phases via using winding numbers. Our work also shows the bulk-corner correspondence that exist between the invariants and the zero modes at the corners. With four zero modes at the corners and a winding number as 2, we conclude that the system has transformed into a second order topological insulator via tuning of the hopping amplitudes.