2011
DOI: 10.1080/09500340.2011.559316
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Amplified optomechanics in a unidirectional ring cavity

Abstract: We investigate optomechanical forces on a nearly lossless scatterer, such as an atom pumped far off-resonance or amicromirror, inside an optical ring cavity. Our model introduces two additional features to the cavity: an isolator is used to prevent circulation and resonant enhancement of the pump laser field and thus to avoid saturation of or damage to the scatterer, and an optical amplifier is used to enhance the effective $Q$-factor of the counterpropagating mode and thus to increase the velocity-dependent f… Show more

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Cited by 8 publications
(9 citation statements)
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“…In the fundamental aspect, our study indicates the novel possibility to actively enhance other important nonlinear COM effects, such as photon blockade [41,42], phonon squeezing [8], and photon-phonon entanglement. In the future, we also plan to study nonlinear OMIT in a system with multiple phonon modes [15] or intrinsic two-level-system defects [43], especially the possibility of enhancing the sensitivity of detecting the inter-mode mechanical coupling or the phonon-defect coupling, by virtue of the actively amplified OMIT spectrum [39,44,45]. , as a function of pump power for the passive-passive system (k g = -1) (a) and the active-passive system with k g = 0.4 (b), 1.0 (c), or 1.6 (d).…”
Section: Resultsmentioning
confidence: 99%
“…In the fundamental aspect, our study indicates the novel possibility to actively enhance other important nonlinear COM effects, such as photon blockade [41,42], phonon squeezing [8], and photon-phonon entanglement. In the future, we also plan to study nonlinear OMIT in a system with multiple phonon modes [15] or intrinsic two-level-system defects [43], especially the possibility of enhancing the sensitivity of detecting the inter-mode mechanical coupling or the phonon-defect coupling, by virtue of the actively amplified OMIT spectrum [39,44,45]. , as a function of pump power for the passive-passive system (k g = -1) (a) and the active-passive system with k g = 0.4 (b), 1.0 (c), or 1.6 (d).…”
Section: Resultsmentioning
confidence: 99%
“…We provide a further focus on the pure coherent coupling in Sec. IV, where we investigate an optomechanical ring cavity system [49][50][51]. We provide an application example where in certain cases this coupling is beneficial for laser cooling of the mechanical oscillator to its ground state.…”
Section: Introductionmentioning
confidence: 99%
“…The standard theory for optomechanical damping would thus predict no damping at all. This is probably the reason why the optomechanics of nanooscillators in ring cavities has been discussed only in few papers so far [9,10]. Please note in this context that oscillators in ring-like Michelson-Sagnac interferometers are equivalent to the MIM setup [11,12].…”
Section: Introductionmentioning
confidence: 99%