Topological properties of the long-range Kitaev chain with Aubry-Andr\'e-Harper modulation

TL;DR

This paper investigates the topological phases of a long-range Kitaev chain with Aubry-André-Harper modulation, revealing how decay rates influence edge modes, topological invariants, and the bulk-boundary correspondence.

Contribution

It introduces a detailed analysis of how algebraic decay in pairing affects topological properties and edge modes in the long-range Kitaev chain with Aubry-André-Harper potential.

Findings

Critical pairing strength determines topological triviality.

Presence of Majorana zero-modes for fast decay of pairing.

Weakening of bulk-boundary correspondence in the long-range system.

Abstract

We present a detailed study of the topological properties of the Kitaev chain with long-range pairing terms and in the presence of an Aubry-Andr\'e-Harper on-site potential. Specifically, we consider algebraically decaying superconducting pairing amplitudes; the exponent of this decay is found to determine a critical pairing strength, below which the chain remains topologically trivial. Above the critical pairing, topological edge modes are observed in the central gap. For sufficiently fast decay of the pairing, these modes are identified as Majorana zero-modes. However, if the pairing term decays slowly, the modes become massive Dirac modes. Interestingly, these massive modes still exhibit a true level crossing at zero energy, which points towards an initimate relation to Majorana physics. We also observe a clear lack of bulk-boundary correspondence in the long-range system, where bulk topological invariants remain constant, while dramatic changes appear in the behavior at the edge of the system. In addition to the central gap around zero energy, the Aubry-Andr\'e-Harper potential also leads to other energy gaps at non-zero energy. As for the analogous short-range model, the edge modes in these gaps can be characterized through a 2D Chern invariant. However, in contrast to the short-range model, this topological invariant does not correspond to the number of edge mode crossings anymore. This provides another example for the weakening of the bulk-boundary correspondence occurring in this model. Finally, we discuss possible realizations of the model with ultracold atoms and condensed matter systems.