Pseudo-chirality: a manifestation of Noether's theorem in non-Hermitian systems

TL;DR

This paper explores how Noether's theorem manifests in non-Hermitian systems through a concept called pseudo-chirality, revealing new constants of motion and their implications for topological lattice systems.

Contribution

It introduces pseudo-chirality as a generalized symmetry in non-Hermitian systems, uncovering new constants of motion and their role in topological phenomena.

Findings

Identification of pseudo-chirality as a symmetry in non-Hermitian systems

Discovery of new constants of motion linked to pseudo-chirality

Implications for topological edge states and lattice size effects

Abstract

Noether's theorem relates constants of motion to the symmetries of the system. Here we investigate a manifestation of Noether's theorem in non-Hermitian systems, where the inner product is defined differently from quantum mechanics. In this framework, a generalized symmetry which we term pseudo-chirality emerges naturally as the counterpart of symmetries defined by a commutation relation in quantum mechanics. Using this observation, we reveal previously unidentified constants of motion in non-Hermitian systems with parity-time and chiral symmetries. We further elaborate the disparate implications of pseudo-chirality induced constant of motion: It signals the pair excitation of a generalized "particle" and the corresponding "hole" but vanishes universally when the pseudo-chiral operator is anti-symmetric. This disparity, when manifested in a non-Hermitian topological lattice with the Landau gauge, depends on whether the lattice size is even or odd. We further discuss previously unidentified symmetries of this non-Hermitian topological system, and we reveal how its constant of motion due to pseudo-chirality can be used as an indicator of whether a pure chiral edge state is excited.