2017
DOI: 10.1364/prj.5.000367
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Optomechanically induced transparency in a spinning resonator

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Cited by 105 publications
(55 citation statements)
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“…Before ending this section, we remark that one mechanical mode coupling to WGC optical modes has been demonstrated experimentally [ 52–55 ] and extended to that containing the optical Sagnac effect. [ 56–58 ] The present work continues the investigation on this topic and focus on the aspect of its nonreciprocal quantum property.…”
Section: Nonreciprocal Mechanical Squeezingmentioning
confidence: 90%
“…Before ending this section, we remark that one mechanical mode coupling to WGC optical modes has been demonstrated experimentally [ 52–55 ] and extended to that containing the optical Sagnac effect. [ 56–58 ] The present work continues the investigation on this topic and focus on the aspect of its nonreciprocal quantum property.…”
Section: Nonreciprocal Mechanical Squeezingmentioning
confidence: 90%
“…In a spinning resonator, the CW or CCW optical mode experiences different refractive indices [70], i.e., n ± = n[1 ± r 2 Ω(n −2 − 1)/c], where n and r 2 denote, respectively, the refractive index and the radius of the resonator, and c is the speed of light in vacuum. As a result, the frequencies of the CW and CCW modes of the resonator experience Sagnac-Fizeau shifts [78,79]. For light propagating in the same, or opposite, direction of the spinning resonator, we have…”
Section: Model and Solutionsmentioning
confidence: 99%
“…Recently novel avenues to achieve nonreciprocity of electromagnetic fields without magnets but using new scattering effects and a new class of materials and metamaterials have been implemented. [ 16–21 ] The examples include dynamic spatiotemporal modulation of parameters, [ 22–25 ] synthetic magnetic field, [ 25–27 ] angular momentum biasing in photonic or acoustic systems, [ 21,28,29 ] nonlinearity, [ 30–33 ] interband photonic transitions, [ 34,35 ] optomechanics, [ 36–40 ] optoacoustics, [ 41,42 ] parity‐time (PT)‐symmetry breaking, [ 43–45 ] unidirectional gain and loss, [ 46–53 ] moving/rotating cavities [ 54–56 ] and emitters, [ 57 ] Doppler‐shift, [ 58 ] chiral light‐matter coupling and valley polarization, [ 59–63 ] and quantum nonlinearity. [ 64–67 ] Furthermore, quantum systems based on superconducting Josephson junctions attract much attention as they hold a great promise for quantum computing.…”
Section: Introductionmentioning
confidence: 99%