2017
DOI: 10.1063/1.4978671
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Synchronization in air-slot photonic crystal optomechanical oscillators

Abstract: In this Letter, we report observations for the optomechanical oscillator (OMO) synchronization in an air-slot photonic crystal (PhC) cavity driven by a single laser source. Two very-close mechanical modes are found in the air-slot PhC OMO cavity and can be locked to each other at drive powers above the threshold with different detunings. The improvement in phase noise (−70 dBc/Hz at 10 kHz offset) for the synchronized OMO is reported as well. The stable frequency tones obtained open a path toward reconfigurabl… Show more

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Cited by 9 publications
(7 citation statements)
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“…When the latter overcomes the internal mechanical friction, a Hopf bifurcation towards a regime of self-induced mechanical oscillations takes place [28,29,30,31,32,33], with a fixed amplitude, and a free running oscillation phase, which may lock to external forces or to other optomechanical oscillators [34]. This mutual phase-locking of self-oscillating resonators is at the basis of optomechanical synchronization, which has been thoroughly investigated both theoretically [5,19,20,35,36,37,38,39,40,41,42], and experimentally [43,44,45,46,47,48,49,50,51,52] under different configurations. The non-linear effects of radiation pressure manifest themselves whenever the mechanical motion produces a cavity frequency shift comparable or larger than the optical linewidth, resulting in a nontrivial modification of the cavity response to the external driving.…”
Section: Introductionmentioning
confidence: 99%
“…When the latter overcomes the internal mechanical friction, a Hopf bifurcation towards a regime of self-induced mechanical oscillations takes place [28,29,30,31,32,33], with a fixed amplitude, and a free running oscillation phase, which may lock to external forces or to other optomechanical oscillators [34]. This mutual phase-locking of self-oscillating resonators is at the basis of optomechanical synchronization, which has been thoroughly investigated both theoretically [5,19,20,35,36,37,38,39,40,41,42], and experimentally [43,44,45,46,47,48,49,50,51,52] under different configurations. The non-linear effects of radiation pressure manifest themselves whenever the mechanical motion produces a cavity frequency shift comparable or larger than the optical linewidth, resulting in a nontrivial modification of the cavity response to the external driving.…”
Section: Introductionmentioning
confidence: 99%
“…Optical backaction in this case counteracts the internal mechanical friction, and when the total effective damping becomes equal to zero, a Hopf bifurcation into a regime of self-induced mechanical oscillations takes place [23,[28][29][30][31][32][33][34]. A fixed amplitude limit cycle is established, with a free running oscillation phase, which may lock to external forces or to other optomechanical oscillators [35], leading to synchronization (see references [12,15,16,22,[36][37][38][39][40][41][42] for theoretical characterizations, and references [17][18][19][20][21]24,[43][44][45][46] for experimental demonstrations in optomechanical and electromechanical devices). In the specific case of the two-membrane-in-the-middle setup of interest here, self-organized synchronization, phase-locking, and the transition between in-phase and antiphase regimes have been qualitatively demonstrated [24], without calibration of the mechanical displacements.…”
Section: Introductionmentioning
confidence: 99%
“…Laser-cooled atoms and quantum interferometry has provided new advances in precision measurements of fundamental constants [1], time [2], forces [3], gravity [4,5], gravitational red-shift [6], and inertial sensing [7], In parallel, recent advances in radiation-pressure driven cavity optomechanics [8,9] have provided new frontiers for laser cooling of mesoscopic systems [10][11][12], chip-scale stable RF sources [13][14][15], phonon lasers [16], induced-transparency through multi-mode interferences [17,18], chaos generation and transfer [19,20], and explorations into potential quantum transductions of microwave, spin, and optical qubits [21,22]. In cavity optomechanics, the optical cavity and mechanical resonator are co-designed to achieve large optomechanical coupling and transduction [9,23].…”
Section: Introductionmentioning
confidence: 99%