Dynamical quantum phase transitions in free-fermion quantum batteries produce nonanalytic singularities in long-time stored energy by making critical momentum modes charge perfectly at specific times.
Heyl, Dynamical quantum phase transitions: A brief survey, Europhysics Letters125, 26001 (2019)
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Periodic driving induces DQPTs in the 1D Ising model via resonance within a phase (linked to Floquet topology) or low-frequency crossing of the critical point due to energy degeneracy.
Different classes of dissipators in coupled quantum Ising models produce either equilibrium-like relaxation with protocol-dependent dynamics or nonequilibrium steady states featuring reentrant symmetry breaking.
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.
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Dynamical Criticality Behind Energy-Storage Singularities in Quantum Batteries
Dynamical quantum phase transitions in free-fermion quantum batteries produce nonanalytic singularities in long-time stored energy by making critical momentum modes charge perfectly at specific times.
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Dynamical Phase Transitions in Periodically Driving 1D Ising Model
Periodic driving induces DQPTs in the 1D Ising model via resonance within a phase (linked to Floquet topology) or low-frequency crossing of the critical point due to energy degeneracy.
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Dissipation Mechanisms and Dissipative Phase Transitions of two coupled Fully Connected Quantum Ising models
Different classes of dissipators in coupled quantum Ising models produce either equilibrium-like relaxation with protocol-dependent dynamics or nonequilibrium steady states featuring reentrant symmetry breaking.
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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.