Physical Review Letters · 2013 · 325 citations · 40 references
Natural SciencesPhysicsDynamical SystemsOpticsQuantum MechanicsDissipative SystemsNonlinear OpticsOptical ResonatorsQuantum DynamicsQuantum OpticsDissipative DynamicsLangevin EquationsMany-body DynamicsMany-body Quantum MechanicsMany-body Quantum SystemsQuantum Many-body SystemsQuantum OptomechanicsWeak Coupling
At each site of an array, a localized mechanical mode interacts with a laser‑driven cavity mode via radiation pressure, and photons and phonons can hop between neighboring sites. We study the nonlinear driven dissipative quantum dynamics of an array of optomechanical systems. We employ a Gutzwiller ansatz and semiclassical Langevin equations on finite lattices, and propose a realistic experimental implementation in optomechanical crystals. The competition between coherent interaction and dissipation yields a rich phase diagram of optical and mechanical many‑body states, with weak coupling producing incoherent mechanical motion and stronger coupling inducing a transition to phase‑coherent mechanical oscillations.
We study the nonlinear driven dissipative quantum dynamics of an array of optomechanical systems. At each site of such an array, a localized mechanical mode interacts with a laser-driven cavity mode via radiation pressure, and both photons and phonons can hop between neighboring sites. The competition between coherent interaction and dissipation gives rise to a rich phase diagram characterizing the optical and mechanical many-body states. For weak intercellular coupling, the mechanical motion at different sites is incoherent due to the influence of quantum noise. When increasing the coupling strength, however, we observe a transition towards a regime of phase-coherent mechanical oscillations. We employ a Gutzwiller ansatz as well as semiclassical Langevin equations on finite lattices, and we propose a realistic experimental implementation in optomechanical crystals.
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