Universal critical timescales in slow non-Hermitian dynamics
arXiv QuantumArchived Apr 03, 2026✓ Full text saved
arXiv:2604.01918v1 Announce Type: new Abstract: Non-Hermitian systems driven along slow parametric loops undergo non-adiabatic transitions whose outcome depends sensitively on the driving speed, yet no explicit formula has been available for the critical timescale $T_{\mathrm{cr}}$ at which these transitions develop. Using a $2\times 2$ Hamiltonian with circular parameter trajectories, we derive $T_{\mathrm{cr}} = \mathcal{G}\,\ln(1/|\Delta|)$ in closed form for non-encircling loops, phase-shift
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✦ AI Summary· Claude Sonnet
Quantum Physics
[Submitted on 2 Apr 2026]
Universal critical timescales in slow non-Hermitian dynamics
Giorgos Pappas, Diego Bautista Avilés, Luis E. F. Foa Torres, Vassos Achilleos
Non-Hermitian systems driven along slow parametric loops undergo non-adiabatic transitions whose outcome depends sensitively on the driving speed, yet no explicit formula has been available for the critical timescale T_{\mathrm{cr}} at which these transitions develop. Using a 2\times 2 Hamiltonian with circular parameter trajectories, we derive T_{\mathrm{cr}} = \mathcal{G}\,\ln(1/|\Delta|) in closed form for non-encircling loops, phase-shifted loops, offset loops, and loops encircling exceptional points, where \mathcal{G} is a geometry-dependent growth factor and \Delta is the instability seed. This formula sharply separates the regime where the system remains in the averagely dominant eigenstate (T< T_{\mathrm{cr}}) from the superadiabatic regime where the instantaneous dominant eigenstate takes over (T> T_{\mathrm{cr}}), resolving the apparent tension between the previous literature. We identify two competing seeds: a geometric Stokes multiplier and the finite-precision floor. When the geometric seed vanishes, precision alone governs the transition, yielding T_{\mathrm{cr}} \propto m\ln\beta, linear in the number of precision bits m. This provides a purely forward-evolution manifestation of precision-induced irreversibility (PIR)~\cite{PIR}, demonstrating that the fundamental limit identified through echo protocols also controls the outcome of slow non-Hermitian dynamics without requiring time reversal. For PT-symmetric energy spectra, T_{\mathrm{cr}} additionally determines the onset of chirality: the dynamics is non-chiral for T< T_{\mathrm{cr}} and chiral for T> T_{\mathrm{cr}}.
Comments: 11 pages, 6 Figures
Subjects: Quantum Physics (quant-ph); Other Condensed Matter (cond-mat.other)
Cite as: arXiv:2604.01918 [quant-ph]
(or arXiv:2604.01918v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2604.01918
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Submission history
From: Vassos Achilleos A [view email]
[v1] Thu, 2 Apr 2026 11:35:16 UTC (3,444 KB)
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