Topological Phase Transition with Larger Winding Number in the Non‐Hermitian Dimerized Lattice.

The topological phase transitions among normal insulator phase, two kinds of topological insulator phases, and topological semimetal phase are shown based on the non‐Hermitian dimerized Su–Schrieffer–Heeger (SSH) model with the nonreciprocal intercell and long‐range hopping. In contrast to the previous work, it is found that the topological insulator phase in the present SSH model can hold the larger non‐Bloch winding number accompanied by exceptional winding of the generalized Brillouin zone around the gap‐closing points. Compared with the usual topological insulator phase in non‐Hermitian SSH model, the topological insulator with the larger winding number owns two pairs of zero energy modes with a distinct form of edge localization in the gap. The physical mechanism of the distinct edge localization for zero energy modes via a equivalent Hermitian version of the non‐Hermitian SSH model is revealed. Additionally, the process of the phase transition is visualized among normal insulator phase, topological insulator phases, and topological semimetal phase in detail via the evolution of the gap‐closing points on the plane of generalized Brillouin zone. This work further verifies the non‐Bloch theory and enrich the investigation about the topologically nontrivial phase with the larger topological invariant in the non‐Hermitian SSH model. [ABSTRACT FROM AUTHOR]