A single-particle dark state in a dissipating spin chain induces universal long-time many-body dynamics with momentum distribution scaling as k sqrt(t) and density decaying as 1/(sqrt(t) log t).
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Exact steady states are derived for interacting dissipative fermionic systems with hidden time-reversal symmetry, revealing a first-order particle density phase transition that survives finite dissipation.
A model-agnostic randomized dissipative cooling protocol drives generic strongly correlated fermionic systems to their low-energy manifold using local ancilla couplings with random energy splittings.
Seeding boundary time crystals induces a measurement-induced phase transition where steady-state entanglement entropy scales with system size N in the seeded phase but decays exponentially otherwise.
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Universal dynamics from a single-particle dark state
A single-particle dark state in a dissipating spin chain induces universal long-time many-body dynamics with momentum distribution scaling as k sqrt(t) and density decaying as 1/(sqrt(t) log t).
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Exact steady states of interacting driven dissipative fermionic systems with hidden time-reversal symmetry
Exact steady states are derived for interacting dissipative fermionic systems with hidden time-reversal symmetry, revealing a first-order particle density phase transition that survives finite dissipation.
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Model-agnostic cooling algorithms for strongly interacting fermions
A model-agnostic randomized dissipative cooling protocol drives generic strongly correlated fermionic systems to their low-energy manifold using local ancilla couplings with random energy splittings.
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Quantum Trajectory Entanglement in Seeded Boundary Time Crystals
Seeding boundary time crystals induces a measurement-induced phase transition where steady-state entanglement entropy scales with system size N in the seeded phase but decays exponentially otherwise.