2020
DOI: 10.1364/prj.8.000143
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Quantum nonreciprocality in quadratic optomechanics

Abstract: We propose to achieve nonreciprocal quantum control of photons in a quadratic optomechanical (QOM) system based on directional nonlinear interactions. We show that by optically pumping the QOM system in one side, the effective QOM coupling can be enhanced significantly in that side, but not for the other side. This, contrary to the intuitive picture, allows the emergence of a nonreciprocal photon blockade in such optomechanical devices with weak single-photon QOM coupling. Our proposal opens up the prospect of… Show more

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Cited by 59 publications
(17 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%
“…Until now, various methods for generation of multiple-photon states have been proposed in atom-coupled photonic waveguides [8][9][10], Rydberg atomic ensembles [11,12], Kerr cavity systems [13], cavity optomechanical systems [14,15], cavity quantum electrodynamics (QED) systems [16], and multiple-level atomic systems [17][18][19][20][21][22][23][24]. Unlike the photon blockade effect [25][26][27][28][29][30][31][32][33][34][35][36][37][38][39], the energy unit of the multiple-photon bundle emission is a bundle of several photons rather than a single photon. In addition, the physical mechanism for multiple-photon bundle emission is a bundle of photons blocking the transmission of the next bundle of photons, rather than n photons blocking the transmission of the (n + 1)th photon.…”
Section: Introductionmentioning
confidence: 99%
“…Up to now, the controllable single-photon states have been extensively studied by using the mechanisms of conventional PB and unconventional PB. The former mechanism requires a strong optical nonlinearity with large enough energy-spectrum anharmonicity in the systems, ranging from cavity quantum electrodynamics (QED) [8][9][10][11][12][13][14][15][16] to circuit QED [17][18][19][20][21], Kerrtype nonlinear systems [7,[22][23][24][25][26][27][28], and optomechanical resonators [29][30][31][32][33][34][35][36]. The latter mechanism relies on the destructive quantum interference by constructing different quantum transition pathways [37][38][39][40][41][42][43].…”
Section: Introductionmentioning
confidence: 99%