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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Coupling ghost modes to dissipative baths generates dynamically effective masses and widths that suppress Ostrogradsky instabilities above a critical coupling via bifurcated dissipative branches and a phase transition.
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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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Dissipative stabilization of Ostrogradsky modes in non-equilibrium field theory
Coupling ghost modes to dissipative baths generates dynamically effective masses and widths that suppress Ostrogradsky instabilities above a critical coupling via bifurcated dissipative branches and a phase transition.