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This research investigates anomalous Gouy-phase behavior in non-Hermitian Dirac systems, establishing it as a sensitive probe for global PT-symmetry-breaking thresholds. The study reveals a counterintuitive mass-dependent crossover between classical and quantum regimes within photonic waveguides featuring gain and loss. These findings offer new theoretical tools for controlling exceptional points and designing advanced photonic devices with precise threshold detection capabilities.
Gouy Phase across PT-Symmetry Breaking in Non-Hermitian Dirac Systems
arXiv:2609.01884v1 Announce Type: new Abstract: We study relativistic beam-like wave packets governed by a quasi-Hermitian massive Dirac Hamiltonian and uncover anomalous Gouy-phase behavior in non-Hermitian dynamics. We show that the Gouy phase provides a sensitive probe of the global $\mathcal{PT}$-symmetry-breaking threshold: it remains purely real in the globally unbroken, quasi-Hermitian regime, while, after crossing the exceptional point, the Gouy phase changes sign and acquires an imaginary component. At the exceptional point, the Gouy-phase variation vanishes in the small-mass limit but becomes maximal for large masses, revealing a counterintuitive crossover from effectively classical to increasingly wave-like quantum behavior. We propose an experimental scheme to measure the components of the non-Hermitian Gouy phase in the broken regime by monitoring the attenuation of a light beam propagating through a lossy waveguide. These results highlight the potential of the non-Hermitian Gouy phase for photonic applications, including the determination of threshold conditions and the design and control of systems with gain and loss.
Abstract:We study relativistic beam-like wave packets governed by a quasi-Hermitian massive Dirac Hamiltonian and uncover anomalous Gouy-phase behavior in non-Hermitian dynamics. We show that the Gouy phase provides a sensitive probe of the global $\mathcal{PT}$-symmetry-breaking threshold: it remains purely real in the globally unbroken, quasi-Hermitian regime, while, after crossing the exceptional point, the Gouy phase changes sign and acquires an imaginary component. At the exceptional point, the Gouy-phase variation vanishes in the small-mass limit but becomes maximal for large masses, revealing a counterintuitive crossover from effectively classical to increasingly wave-like quantum behavior. We propose an experimental scheme to measure the components of the non-Hermitian Gouy phase in the broken regime by monitoring the attenuation of a light beam propagating through a lossy waveguide. These results highlight the potential of the non-Hermitian Gouy phase for photonic applications, including the determination of threshold conditions and the design and control of systems with gain and loss.
arXiv:2609.01884 [quant-ph]
(or arXiv:2609.01884v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2609.01884 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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