Chinese Optics Letters, Volume. 16, Issue 11, 111201(2018)

Effects of Casimir force on high-order sideband generation in an optomechanical system

Jie Yao, Yafei Yu*, and Zhiming Zhang**
Author Affiliations
  • Guangdong Provincial Key Laboratory of Nanophotonic Functional Materials and Devices (School of Information and Optoelectronic Science and Engineering); Guangdong Provincial Key Laboratory of Quantum Engineering and Quantum Materials, South China Normal University, Guangzhou 510006, China
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    Figures & Tables(4)
    Sketch of the system.
    Intracavity steady-state mean photon number |as|2 varies with (a) the sphere–mirror separation and (b) the power of the controlling field. The parameters used are m=145 ng, ωm=2π×947 kHz, Γm=2π×141 Hz, R=150 nm, κ=2π×215 Hz, ωl=2 πc/λ, λ=1064 nm, g=2π×70 GHz/μm, and Δl=ωm. In addition, (a) Pl=10 μW and (b) d=2 nm.
    Output spectra for different values of the sphere–mirror separation d: (a) d=∞, (b) d=2 nm, (c) d=1.8 nm, and (d) d=1.5 nm. We use εp=εl/2. The power of the controlling field is Pl=30 μW. The other parameters are the same as in Fig. 2.
    Output spectra for different values of the optomechanical coupling strength g: (a) g=g0, (b) g=2g0, (c) g=3g0, (d) g=4g0, here g0=70 GHz/μm. The sphere–mirror separation is d=2 nm. The other parameters are the same as in Fig. 2.
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    Jie Yao, Yafei Yu, Zhiming Zhang. Effects of Casimir force on high-order sideband generation in an optomechanical system[J]. Chinese Optics Letters, 2018, 16(11): 111201

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    Paper Information

    Category: Instrumentation, measurement, and metrology

    Received: Aug. 9, 2018

    Accepted: Sep. 29, 2018

    Posted: Sep. 29, 2018

    Published Online: Nov. 11, 2018

    The Author Email: Yafei Yu (yfyuks@hotmail.com), Zhiming Zhang (zmzhang@scnu.edu.cn)

    DOI:10.3788/COL201816.111201

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