Laser Theory for Optomechanics: Limit Cycles in the Quantum Regime

Optomechanical systems can exhibit self-sustained limit cycles where the quantum state of the mechanical resonator possesses nonclassical characteristics such as a strongly negative Wigner density, as was shown recently in a numerical study by Qian et al. [Phys. Rev. Lett. 109, 253601 (2012)]. Here,...

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Main Authors: Niels Lörch, Jiang Qian, Aashish Clerk, Florian Marquardt, Klemens Hammerer
Format: Article
Language:English
Published: American Physical Society 2014-01-01
Series:Physical Review X
Online Access:http://doi.org/10.1103/PhysRevX.4.011015
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spelling doaj-6442e73fec0448439c9fd039f8a151782020-11-25T01:51:10ZengAmerican Physical SocietyPhysical Review X2160-33082014-01-014101101510.1103/PhysRevX.4.011015Laser Theory for Optomechanics: Limit Cycles in the Quantum RegimeNiels LörchJiang QianAashish ClerkFlorian MarquardtKlemens HammererOptomechanical systems can exhibit self-sustained limit cycles where the quantum state of the mechanical resonator possesses nonclassical characteristics such as a strongly negative Wigner density, as was shown recently in a numerical study by Qian et al. [Phys. Rev. Lett. 109, 253601 (2012)]. Here, we derive a Fokker-Planck equation describing mechanical limit cycles in the quantum regime that correctly reproduces the numerically observed nonclassical features. The derivation starts from the standard optomechanical master equation and is based on techniques borrowed from the laser theory due to Haake and Lewenstein. We compare our analytical model with numerical solutions of the master equation based on Monte Carlo simulations and find very good agreement over a wide and so far unexplored regime of system parameters. As one main conclusion, we predict negative Wigner functions to be observable even for surprisingly classical parameters, i.e., outside the single-photon strong-coupling regime, for strong cavity drive and rather large limit-cycle amplitudes. The approach taken here provides a natural starting point for further studies of quantum effects in optomechanics.http://doi.org/10.1103/PhysRevX.4.011015
collection DOAJ
language English
format Article
sources DOAJ
author Niels Lörch
Jiang Qian
Aashish Clerk
Florian Marquardt
Klemens Hammerer
spellingShingle Niels Lörch
Jiang Qian
Aashish Clerk
Florian Marquardt
Klemens Hammerer
Laser Theory for Optomechanics: Limit Cycles in the Quantum Regime
Physical Review X
author_facet Niels Lörch
Jiang Qian
Aashish Clerk
Florian Marquardt
Klemens Hammerer
author_sort Niels Lörch
title Laser Theory for Optomechanics: Limit Cycles in the Quantum Regime
title_short Laser Theory for Optomechanics: Limit Cycles in the Quantum Regime
title_full Laser Theory for Optomechanics: Limit Cycles in the Quantum Regime
title_fullStr Laser Theory for Optomechanics: Limit Cycles in the Quantum Regime
title_full_unstemmed Laser Theory for Optomechanics: Limit Cycles in the Quantum Regime
title_sort laser theory for optomechanics: limit cycles in the quantum regime
publisher American Physical Society
series Physical Review X
issn 2160-3308
publishDate 2014-01-01
description Optomechanical systems can exhibit self-sustained limit cycles where the quantum state of the mechanical resonator possesses nonclassical characteristics such as a strongly negative Wigner density, as was shown recently in a numerical study by Qian et al. [Phys. Rev. Lett. 109, 253601 (2012)]. Here, we derive a Fokker-Planck equation describing mechanical limit cycles in the quantum regime that correctly reproduces the numerically observed nonclassical features. The derivation starts from the standard optomechanical master equation and is based on techniques borrowed from the laser theory due to Haake and Lewenstein. We compare our analytical model with numerical solutions of the master equation based on Monte Carlo simulations and find very good agreement over a wide and so far unexplored regime of system parameters. As one main conclusion, we predict negative Wigner functions to be observable even for surprisingly classical parameters, i.e., outside the single-photon strong-coupling regime, for strong cavity drive and rather large limit-cycle amplitudes. The approach taken here provides a natural starting point for further studies of quantum effects in optomechanics.
url http://doi.org/10.1103/PhysRevX.4.011015
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