Boundary time crystals emerge from non-reciprocal operator transport in an irreducible tensor representation of the Liouvillian, unifying collective precession, relaxation, and BTC phases via delocalized eigenmodes.
Wilczek, Quantum Time Crystals, Phys
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Exact asymptotic wavefunction for arbitrary spin s in the time-dependent Richardson-Gaudin model is derived independently per spin size, yielding a non-thermal steady state outside the natural GGE with mean-field exact for finite products of distinct-site spin operators.
A kinetic uncertainty relation is analytically derived for many-body collective dissipation, revealing that collective interactions enable precision to scale with particle number N.
Review summarizing three distinct time crystalline states in cavity-BEC systems, characterized by cavity mode correlations and condensate momentum modes.
citing papers explorer
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Operator Space Transport and the Emergence of Boundary Time Crystals
Boundary time crystals emerge from non-reciprocal operator transport in an irreducible tensor representation of the Liouvillian, unifying collective precession, relaxation, and BTC phases via delocalized eigenmodes.
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Higher spin Richardson-Gaudin model with time-dependent coupling: Exact dynamics
Exact asymptotic wavefunction for arbitrary spin s in the time-dependent Richardson-Gaudin model is derived independently per spin size, yielding a non-thermal steady state outside the natural GGE with mean-field exact for finite products of distinct-site spin operators.
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Kinetic Uncertainty Relation in Collective Dissipative Quantum Many-Body Systems
A kinetic uncertainty relation is analytically derived for many-body collective dissipation, revealing that collective interactions enable precision to scale with particle number N.
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Time crystals in cavity-BEC systems
Review summarizing three distinct time crystalline states in cavity-BEC systems, characterized by cavity mode correlations and condensate momentum modes.