2009
DOI: 10.1002/prop.200900074
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Parametric self pulsing in a quantum opto‐mechanical system

Abstract: We describe an opto-mechanical system in which the coupling between optical and mechanical degrees of freedom takes the form of a fully quantised third-order parametric interaction. Two physical realisations are proposed: a harmonically trapped atom in a standing wave and the 'membrane in the middle' model. The dominant resonant interaction corresponds to a stimulated Raman process in which two phonons are converted into a single cavity photon. We show that this system can exhibit a stable limit-cycle in which… Show more

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Cited by 14 publications
(11 citation statements)
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“…Finally, since our scheme is based only on interacting bosonic fields, its applications are not restricted to optical systems. It could also be implemented in optomechanical, electromechanical and superconducting systems where extremely strong intrinsic nonlinearities involving vibrational [39][40][41] or matter-based [42,43] degrees of freedom are more readily available. two degenerate and indistinguishable photons can be deterministically separated into different modes via a "reverse Hong-Ou-Mandel"-type interaction at a beam splitter (|2, 0 + |0, 2 → |1, 1 ).…”
Section: Discussionmentioning
confidence: 99%
“…Finally, since our scheme is based only on interacting bosonic fields, its applications are not restricted to optical systems. It could also be implemented in optomechanical, electromechanical and superconducting systems where extremely strong intrinsic nonlinearities involving vibrational [39][40][41] or matter-based [42,43] degrees of freedom are more readily available. two degenerate and indistinguishable photons can be deterministically separated into different modes via a "reverse Hong-Ou-Mandel"-type interaction at a beam splitter (|2, 0 + |0, 2 → |1, 1 ).…”
Section: Discussionmentioning
confidence: 99%
“…3. We do this calculation for the case of a single group of nano-mechanical resonators following the procedure of [29]. For a single group, using the dimensionless notation where we have re-scaled the coupling coefficients and time by the cavity dissipation rate κ, we have the stochastic differential equations of motion corresponding to the Fokker-Planck like equation (55)…”
Section: Quantum Spectramentioning
confidence: 99%
“…For a single oscillator, this conversion is completely eliminated by operating at a point for which the resonator frequency is insensitive to the amplitude [17], and this approach can be generalized to achieve amplitude-phase detachment in our system as well. At low enough temperatures the contribution of quantum noise to the phase diffusion becomes relevant, and can be calculated as it was done in [18]. …”
mentioning
confidence: 99%