Quantum jump correlations and waiting-time distributions in long-range dissipative spins display clear signatures of the paramagnetic-to-ferromagnetic transition when analyzed with tilted Lindbladian, cluster mean-field, and cumulant expansion methods.
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UNVERDICTED 4representative citing papers
Aligning an exceptional point with a dissipative phase transition in an extended open Dicke model amplifies critical fluctuations and modifies critical exponents through EP-induced Jordan-block dynamics.
Intrinsic dimension of quantum trajectories serves as an unsupervised probe sensitive to chaos, integrability, and ergodicity breaking in dissipative quantum systems.
Numerical quench dynamics in 1D N-flavor Gross-Neveu lattice fermions show order-parameter equilibration consistent with ETH in the thermodynamic limit and GGE description, while finite-momentum correlations equilibrate only with nonzero reservoir coupling γ.
citing papers explorer
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Quantum jump correlations in long-range dissipative spin systems via cluster and cumulant expansions
Quantum jump correlations and waiting-time distributions in long-range dissipative spins display clear signatures of the paramagnetic-to-ferromagnetic transition when analyzed with tilted Lindbladian, cluster mean-field, and cumulant expansion methods.
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Enhanced dissipative criticality at an exceptional point
Aligning an exceptional point with a dissipative phase transition in an extended open Dicke model amplifies critical fluctuations and modifies critical exponents through EP-induced Jordan-block dynamics.
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Complexity of Quantum Trajectories
Intrinsic dimension of quantum trajectories serves as an unsupervised probe sensitive to chaos, integrability, and ergodicity breaking in dissipative quantum systems.
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Post-quench relaxation dynamics of Gross-Neveu lattice fermions
Numerical quench dynamics in 1D N-flavor Gross-Neveu lattice fermions show order-parameter equilibration consistent with ETH in the thermodynamic limit and GGE description, while finite-momentum correlations equilibrate only with nonzero reservoir coupling γ.