2015
DOI: 10.1088/0031-8949/2015/t165/014003
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Large parametric amplification in an optomechanical system

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Cited by 2 publications
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“…At the parametric instability point, where the backaction-induced mechanical gain overcomes mechanical loss, mechanical self-oscillations start [8], [9], [10], and the system enters into a nonlinear regime. This regime is a prerequisite to study collective phenomena such as synchronization and frequency locking [11], [12], [13], [14], [15].…”
Section: Introductionmentioning
confidence: 99%
“…At the parametric instability point, where the backaction-induced mechanical gain overcomes mechanical loss, mechanical self-oscillations start [8], [9], [10], and the system enters into a nonlinear regime. This regime is a prerequisite to study collective phenomena such as synchronization and frequency locking [11], [12], [13], [14], [15].…”
Section: Introductionmentioning
confidence: 99%