Tuning a photonic-crystal bandgap in a driven Kerr microresonator switches the soliton spectrum between a uniform-power Mott-insulator comb and a non-uniform superfluid comb with phase coherence.
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4 Pith papers cite this work. Polarity classification is still indexing.
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Bilayer Kagome spin ice on quantum annealer exhibits sharp Ice-II transition at J_perp/J1 ≈ 0.042 with independent control of monopoles via quantum drive and charge order via interlayer coupling.
The work identifies two distinct topological phases in bond-alternating spin-1 nanographene chains and proposes two specific molecular candidates whose phases can be distinguished by inelastic electron tunneling spectroscopy.
In Josephson junction chains, non-resonant two-into-two scattering dominates equilibrium plasmon decay rates while strong driving induces a crossover to a qualitatively different non-equilibrium steady state.
citing papers explorer
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Nanophotonic control of collective many-body states in Kerr solitons
Tuning a photonic-crystal bandgap in a driven Kerr microresonator switches the soliton spectrum between a uniform-power Mott-insulator comb and a non-uniform superfluid comb with phase coherence.
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Competing interlayer charge order and quantum monopole reorganization in bilayer Kagome spin ice via quantum annealing
Bilayer Kagome spin ice on quantum annealer exhibits sharp Ice-II transition at J_perp/J1 ≈ 0.042 with independent control of monopoles via quantum drive and charge order via interlayer coupling.
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Two topological phases in exchange alternating spin-1 nanographene chains
The work identifies two distinct topological phases in bond-alternating spin-1 nanographene chains and proposes two specific molecular candidates whose phases can be distinguished by inelastic electron tunneling spectroscopy.
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Plasmon decay and non-equilibrium steady states in Josephson junction chains
In Josephson junction chains, non-resonant two-into-two scattering dominates equilibrium plasmon decay rates while strong driving induces a crossover to a qualitatively different non-equilibrium steady state.