A dissipation gradient plus detuning ramp selects a resonant pinned density front in 2D driven-dissipative Bose-Hubbard lattice simulations, producing tunable depinning, pattern locking, and chaos.
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Mass imbalance and Coulomb strength control a BCS-BEC crossover in polaritonic condensates, with semiconductors favoring BEC-like excitonic states at low density and semimetals favoring BCS pairing except at strong interactions and large imbalance.
KPZ scaling in arrays of polariton condensates originates from fluctuations of Goldstone modes caused by U(1) symmetry breaking.
citing papers explorer
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Dissipation-Selected Resonant Fronts in a Driven-Dissipative Bose-Hubbard Lattice
A dissipation gradient plus detuning ramp selects a resonant pinned density front in 2D driven-dissipative Bose-Hubbard lattice simulations, producing tunable depinning, pattern locking, and chaos.
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BCS-BEC crossover of polaritonic condensates in mass-imbalanced semimetal/semiconductor microcavities
Mass imbalance and Coulomb strength control a BCS-BEC crossover in polaritonic condensates, with semiconductors favoring BEC-like excitonic states at low density and semimetals favoring BCS pairing except at strong interactions and large imbalance.
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The origin of KPZ-scaling in arrays of polariton condensates
KPZ scaling in arrays of polariton condensates originates from fluctuations of Goldstone modes caused by U(1) symmetry breaking.