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This research reveals a critical size-dependent instability in periodic $\mathcal{PT}$-symmetric systems where enlarging the structure to access richer band phenomena paradoxically lowers the threshold for dynamical failure. The derived closed-form instability threshold indicates that many standard non-Hermitian transport effects, such as reflectionless transport and coherent perfect absorbers, may exist only within a dynamically unstable regime for large $N$. Consequently, engineers designing wave-tailoring platforms must account for finite-size stability limits rather than relying solely on stationary band theory.
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Size-dependent dynamical instability of periodic $\mathcal{PT}$-symmetric scattering systems

arXiv2 min read

arXiv:2605.10657v2 Announce Type: replace Abstract: While periodic $\mathcal{PT}$-symmetric structures offer a versatile platform for wave tailoring, their scattering responses are typically analyzed using stationary methods that presume dynamical stability. This assumption fails when time-growing bound states emerge, signaling a dynamical instability. Here, we analytically derive the instability threshold for a $\mathcal{PT}$-symmetric chain of $N$ unit cells with gain/loss strength $\gamma$. Our $S$-matrix analysis yields a closed-form threshold, $\gamma_c = 2\sin[\pi/(4N)]$, which scales as $\mathcal{O}(1/N)$ and vanishes in the thermodynamic limit. Consequently, enlarging such structures to access richer stationary band phenomena paradoxically triggers instability at weaker gain/loss. As confirmed by time-domain simulations, exceeding $\gamma_c$ causes exponentially growing bound states to overwhelm the system, rendering standard Bloch-wave descriptions physically irrelevant. Evaluated against this size-dependent threshold, many hallmarks of large $\mathcal{PT}$-symmetric structures, including gain-loss-induced localization, reflectionless transport, and coherent perfect absorbers and lasers, are found to lie within the dynamically unstable regime. Our findings thus establish that physical transport in non-Hermitian periodic systems is governed by a fundamental interplay between stationary band theory and finite-size stability limits.

Abstract:While periodic $\mathcal{PT}$-symmetric structures offer a versatile platform for wave tailoring, their scattering responses are typically analyzed using stationary methods that presume dynamical stability. This assumption fails when time-growing bound states emerge, signaling a dynamical instability. Here, we analytically derive the instability threshold for a $\mathcal{PT}$-symmetric chain of $N$ unit cells with gain/loss strength $\gamma$. Our $S$-matrix analysis yields a closed-form threshold, $\gamma_c = 2\sin[\pi/(4N)]$, which scales as $\mathcal{O}(1/N)$ and vanishes in the thermodynamic limit. Consequently, enlarging such structures to access richer stationary band phenomena paradoxically triggers instability at weaker gain/loss. As confirmed by time-domain simulations, exceeding $\gamma_c$ causes exponentially growing bound states to overwhelm the system, rendering standard Bloch-wave descriptions physically irrelevant. Evaluated against this size-dependent threshold, many hallmarks of large $\mathcal{PT}$-symmetric structures, including gain-loss-induced localization, reflectionless transport, and coherent perfect absorbers and lasers, are found to lie within the dynamically unstable regime. Our findings thus establish that physical transport in non-Hermitian periodic systems is governed by a fundamental interplay between stationary band theory and finite-size stability limits.

Quantum Physics (quant-ph); Optics (physics.optics)

arXiv:2605.10657 [quant-ph]

(or arXiv:2605.10657v2 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2605.10657 Focus to learn more arXiv-issued DOI via DataCite

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Full text under the publisher's open licence · 263 words

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