Topology in a PT-symmetric SSH quantum battery produces an edge exceptional point at smaller gain-loss strength, yielding better transient and long-time charging, stored energy, and extractable work than the trivial configuration.
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Superradiant phase transition in the anisotropic Rabi model arises from competition among three Hamiltonian patterns and is equivalently simulated by a parametrically-driven Jaynes-Cummings model where excitation energies vanish at criticality.
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Topological enhancement of a PT-symmetric Su-Schrieffer-Heeger quantum battery
Topology in a PT-symmetric SSH quantum battery produces an edge exceptional point at smaller gain-loss strength, yielding better transient and long-time charging, stored energy, and extractable work than the trivial configuration.
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Dissecting the superradiant phase transition in the anisotropic Rabi model: Pattern competition and cavity-QED simulation
Superradiant phase transition in the anisotropic Rabi model arises from competition among three Hamiltonian patterns and is equivalently simulated by a parametrically-driven Jaynes-Cummings model where excitation energies vanish at criticality.