• Laser & Optoelectronics Progress
  • Vol. 57, Issue 19, 191201 (2020)
Jing Wang*
Author Affiliations
  • College of Physics, Tonghua Normal University, Tonghua, Jilin 134001, China
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    DOI: 10.3788/LOP57.191201 Cite this Article Set citation alerts
    Jing Wang. Nonreciprocity in a Three-Cavity Optomechanical System[J]. Laser & Optoelectronics Progress, 2020, 57(19): 191201 Copy Citation Text show less
    Schematic of the system
    Fig. 1. Schematic of the system
    Transmission amplitudes T12 and T21 versus normalized detuning x/κc1 for different phase differences. (a) θ=-π/2; (b) θ=0; (c) θ=π/2; (d) θ=π
    Fig. 2. Transmission amplitudes T12 and T21 versus normalized detuning x/κc1 for different phase differences. (a) θ=-π/2; (b) θ=0; (c) θ=π/2; (d) θ
    Transmission amplitudes T12 and T21 versus phase difference θ when normalized detuning is 0
    Fig. 3. Transmission amplitudes T12 and T21 versus phase difference θ when normalized detuning is 0
    Transmission amplitudes T12 and T21 versus effective optomechanical coupling intensity G2/G1
    Fig. 4. Transmission amplitudes T12 and T21 versus effective optomechanical coupling intensity G2/G1
    Transmission amplitudes T12 and T21 versus normalized detuning x/κc1 for different cavity damping rates. (a) κc2=15; (b) κc2=1; (c) κc2=0.5; (d) κc2=0.25
    Fig. 5. Transmission amplitudes T12 and T21 versus normalized detuning x/κc1 for different cavity damping rates. (a) κc2=15; (b) κc2=1; (c) κc2=0.5; (d) κc2=0.25
    Jing Wang. Nonreciprocity in a Three-Cavity Optomechanical System[J]. Laser & Optoelectronics Progress, 2020, 57(19): 191201
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