Impurity-induced loss bursts from anomalous scale-free localization in a non-Hermitian dissipative lattice

TL;DR

This paper uncovers impurity-induced loss bursts linked to anomalous scale-free localization in a non-Hermitian lattice, revealing how impurity strength tunes boundary conditions and affects dissipation dynamics.

Contribution

It introduces a novel impurity-induced loss burst mechanism connected to anomalous scale-free localization in a non-Hermitian lattice model.

Findings

Impurity strength tunes between different effective boundary conditions.

Eigenstates exhibit scale-free localization with energy-dependent Lyapunov exponents.

Loss bursts are strongly enhanced near impurity-generated effective boundaries.

Abstract

We identify anomalous scale-free localization and the associated impurity-induced loss bursts in a non-Hermitian dissipative cross-stitch lattice. By a local basis rotation, the model is mapped onto an effective non-Hermitian Su-Schrieffer-Heeger lattice, where local impurities act as tunable effective boundaries. For the parameter choice considered here, tuning the impurity strength $\eta$ connects two effective open-boundary-condition-like limits, reached for $\eta\to0$ and $\eta\to\infty$, through generalized-boundary-condition regimes and the impurity-free periodic-boundary-condition point at $\eta=1$. For finite $\eta\notin\{0,1\}$, the spectral loops remain separated from the real-energy axis, while the eigenstates exhibit scale-free localization pinned by the impurity. Unlike conventional impurity-induced scale-free localization, the Lyapunov exponent depends explicitly on the eigenenergy, making the localization strength eigenstate dependent. We further show that this anomalous eigenmode structure produces an impurity-induced loss burst: the long-time integrated dissipation probability is strongly enhanced near an impurity-generated effective boundary even when the initial wave packet is far away. In the single-impurity case, the burst region consists of the impurity site and its adjacent effective-boundary site, and the effect occurs without imaginary-gap closing. For multiple impurities, local burst regions emerge around all impurities, while the dominant burst boundary is selected by the initial wave-packet position and the nonreciprocal drift direction. These results connect anomalous scale-free localization with controllable dissipation dynamics in non-Hermitian lattices.