• Chinese Optics Letters
  • Vol. 20, Issue 6, 062701 (2022)
Jiang-Shan Tang1、2, Lei Tang1, and Keyu Xia1、2、*
Author Affiliations
  • 1College of Engineering and Applied Sciences, National Laboratory of Solid State Microstructures, and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210023, China
  • 2School of Physics, Nanjing University, Nanjing 210023, China
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    DOI: 10.3788/COL202220.062701 Cite this Article Set citation alerts
    Jiang-Shan Tang, Lei Tang, Keyu Xia. Three methods for the single-photon transport in a chiral cavity quantum electrodynamics system[J]. Chinese Optics Letters, 2022, 20(6): 062701 Copy Citation Text show less
    Schematic of a chiral QE-microresonator system. A two-level QE is coupled to a whispering-gallery mode microresonator in a chiral way to form the QE-microresonator system. A waveguide is side coupled to the microresonator as input and output ports. A scatterer on the microresonator is considered to introduce backscattering. The arrows represent the propagating direction of a single photon for an input to port 1 (green) or port 2 (red).
    Fig. 1. Schematic of a chiral QE-microresonator system. A two-level QE is coupled to a whispering-gallery mode microresonator in a chiral way to form the QE-microresonator system. A waveguide is side coupled to the microresonator as input and output ports. A scatterer on the microresonator is considered to introduce backscattering. The arrows represent the propagating direction of a single photon for an input to port 1 (green) or port 2 (red).
    Transmission spectra of a waveguide coupled with a microresonator. The blue solid, red dashed, and green dotted curves are calculated by the TM, ME, and SPT methods, respectively. The settings in the following figures are the same: (a) in the absence of backscattering, (b) and (c) in presence of the backscattering with strengths h = κin and h = 10κin, respectively. See Sec. 3 for other parameters.
    Fig. 2. Transmission spectra of a waveguide coupled with a microresonator. The blue solid, red dashed, and green dotted curves are calculated by the TM, ME, and SPT methods, respectively. The settings in the following figures are the same: (a) in the absence of backscattering, (b) and (c) in presence of the backscattering with strengths h = κin and h = 10κin, respectively. See Sec. 3 for other parameters.
    Transmission spectra for a chiral QE-microresonator system without considering the backscattering: (a)–(c) Γ = 0.1γ, Γ = γ, and Γ = 100γ, respectively.
    Fig. 3. Transmission spectra for a chiral QE-microresonator system without considering the backscattering: (a)–(c) Γ = 0.1γ, Γ = γ, and Γ = 100γ, respectively.
    Transmission spectra for a chiral QE-microresonator system with the QE and the scatterer: (a) Γ = 100γ, h = κin and (b) Γ = 100γ, h = 10κin.
    Fig. 4. Transmission spectra for a chiral QE-microresonator system with the QE and the scatterer: (a) Γ = 100γ, h = κin and (b) Γ = 100γ, h = 10κin.
    (a) Transmission spectra for different driving amplitudes αin (corresponding to different pump powers), where the blue solid curve is calculated by the TM method, and the green dash-dotted curve (the red dashed curve, the purple dotted curve) is calculated by the ME method, with αin/κtol=0.1 (αin/κtol=0.5, αin/κtol=1). (b) Transmission spectra as a function of αin at different decay rates, where Γ = γ (the blue solid curve) and Γ = 100γ (the red dash-dotted curve) correspond to weak and strong coupling, respectively. Other parameters are κex = κin = 0.5κtol, γ/κtol = 1 × 10−4, g/κtol = 1, and h = κin.
    Fig. 5. (a) Transmission spectra for different driving amplitudes αin (corresponding to different pump powers), where the blue solid curve is calculated by the TM method, and the green dash-dotted curve (the red dashed curve, the purple dotted curve) is calculated by the ME method, with αin/κtol=0.1 (αin/κtol=0.5, αin/κtol=1). (b) Transmission spectra as a function of αin at different decay rates, where Γ = γ (the blue solid curve) and Γ = 100γ (the red dash-dotted curve) correspond to weak and strong coupling, respectively. Other parameters are κex = κin = 0.5κtol, γ/κtol = 1 × 10−4, g/κtol = 1, and h = κin.
    Jiang-Shan Tang, Lei Tang, Keyu Xia. Three methods for the single-photon transport in a chiral cavity quantum electrodynamics system[J]. Chinese Optics Letters, 2022, 20(6): 062701
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