2018
DOI: 10.1103/physreva.97.013805
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Quantum reservoir engineering through quadratic optomechanical interaction in the reversed dissipation regime

Abstract: We explore the electromagnetic field coupled to a mechanical resonator via quadratic optomechanical interaction in the reversed dissipation regime where the mechanical damping rate is much larger than the cavity field dissipation rate. It is shown that in this regime, the cavity field effectively acquires an additional reservoir which is conditioned by the temperature of the mechanical bath as well as the mechanical damping rate. We analytically find the steady-state mean photon number and the critical tempera… Show more

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Cited by 16 publications
(8 citation statements)
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References 38 publications
(55 reference statements)
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“…In our scheme, this is achieved by placing an array of membranes in the middle of an optical cavity so that the interaction between the optical and mechanical mode is proportional to the square of the displacement. By making use of the adiabatic approximation, we can treat the optical field as a controllable reservoir [37,38], which is quite different from the biological systems where the two-phonon processes are determined by the environment. Analytical and numerical methods show that the critical optomechanical coupling strength required to achieve the Fröhlich condensate scales as N 3 (N is the number of membranes).…”
Section: Introductionmentioning
confidence: 99%
“…In our scheme, this is achieved by placing an array of membranes in the middle of an optical cavity so that the interaction between the optical and mechanical mode is proportional to the square of the displacement. By making use of the adiabatic approximation, we can treat the optical field as a controllable reservoir [37,38], which is quite different from the biological systems where the two-phonon processes are determined by the environment. Analytical and numerical methods show that the critical optomechanical coupling strength required to achieve the Fröhlich condensate scales as N 3 (N is the number of membranes).…”
Section: Introductionmentioning
confidence: 99%
“…Many efforts have been invested in the single-photon strong-coupling regime of linear optomechanics both theoretically [26][27][28][29][30][31][32][33][34][35][36] and experimentally [37][38][39][40]. In recent years, much attention has been paid to the study of quadratic optomechanical systems [41][42][43][44][45][46][47][48][49][50][51][52][53]. A few methods have been suggested to enhance the quadratic coupling strength of optomechanical systems [54][55][56].…”
Section: Introductionmentioning
confidence: 99%
“…In practical, most optomechanical systems naturally support the multimodes [4,[38][39][40], and these modes can be excited by polychromatic laser drive [41]. With the advantages of multiple degrees in multimode optomechanical systems [42], dissipation engineering [43] holds huge potential in all-optical information processing [32,44,45], where two or more mechanical or optical modes lead to a wealth of different possible schemes.…”
Section: Introductionmentioning
confidence: 99%