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This research advances the simulation of open quantum systems by establishing exact steady-state balance relations within normal Lindblad frameworks, offering new insights into how stochastic dynamics recover orthogonal relaxation modes without transient amplification. The work clarifies the trajectory-level mechanisms underlying Liouvillian normality and demonstrates that exceptional points are excluded in these specific generators, which is critical for improving efficiency in large-scale quantum system modeling.
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From normal Lindbladians to non-normal quantum trajectories

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arXiv:2608.04775v1 Announce Type: new Abstract: Efficient simulation of Markovian open quantum systems remains a central challenge because the density-matrix description grows exponentially with system size. Quantum trajectory methods provide an alternative by replacing mixed-state evolution with stochastic pure-state realizations. Here we investigate this framework for normal Lindblad generators, whose orthogonal eigenoperator decomposition precludes transient amplification. By decomposing the Lindbladian into deterministic smooth and stochastic jump contributions, we derive an exact steady-state balance relation that identifies the interplay between these processes as the mechanism underlying Liouvillian normality. We further show that normal Lindbladians exclude exceptional points and that, although individual quantum trajectories generally exhibit stochastic coupling between Liouvillian eigenmodes, these couplings cancel upon ensemble averaging, recovering independent orthogonal relaxation modes. These results provide a trajectory-level interpretation of Liouvillian normality and clarify how a global property of the Lindblad generator is realized through stochastic quantum dynamics.

Abstract:Efficient simulation of Markovian open quantum systems remains a central challenge because the density-matrix description grows exponentially with system size. Quantum trajectory methods provide an alternative by replacing mixed-state evolution with stochastic pure-state realizations. Here we investigate this framework for normal Lindblad generators, whose orthogonal eigenoperator decomposition precludes transient amplification. By decomposing the Lindbladian into deterministic smooth and stochastic jump contributions, we derive an exact steady-state balance relation that identifies the interplay between these processes as the mechanism underlying Liouvillian normality. We further show that normal Lindbladians exclude exceptional points and that, although individual quantum trajectories generally exhibit stochastic coupling between Liouvillian eigenmodes, these couplings cancel upon ensemble averaging, recovering independent orthogonal relaxation modes. These results provide a trajectory-level interpretation of Liouvillian normality and clarify how a global property of the Lindblad generator is realized through stochastic quantum dynamics.

arXiv:2608.04775 [quant-ph]

(or arXiv:2608.04775v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2608.04775 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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