• Acta Physica Sinica
  • Vol. 69, Issue 5, 054203-1 (2020)
Jun-Wen Luo, De-Wei Wu*, Qiang Miao, and Tian-Li Wei
Author Affiliations
  • Information and Navigation College, Air Force Engineering University, Xi’an 710077, China
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    DOI: 10.7498/aps.69.20191735 Cite this Article
    Jun-Wen Luo, De-Wei Wu, Qiang Miao, Tian-Li Wei. Research progress in non-classical microwave states preparation based on cavity optomechanical system[J]. Acta Physica Sinica, 2020, 69(5): 054203-1 Copy Citation Text show less
    Schematic of Fabry-Perot cavity[30].
    Fig. 1. Schematic of Fabry-Perot cavity[30].
    Cavity optomechanical systems with different mecha-nical vibration frequencies and masses[39].
    Fig. 2. Cavity optomechanical systems with different mecha-nical vibration frequencies and masses[39].
    Schematic of Fabry-Perot interferometer.
    Fig. 3. Schematic of Fabry-Perot interferometer.
    Schematic of proposal from Vitali’s group[43].
    Fig. 4. Schematic of proposal from Vitali’s group[43].
    Schematic of proposal from Bitarafan[45].
    Fig. 5. Schematic of proposal from Bitarafan[45].
    Experimental setup of F-P cavity with levitated particle[47].
    Fig. 6. Experimental setup of F-P cavity with levitated particle[47].
    Illustration of whispering gallery mode.
    Fig. 7. Illustration of whispering gallery mode.
    (a) Structures of the first whispering gallery mode cavity[48]; (b) its enhanced version[49].
    Fig. 8. (a) Structures of the first whispering gallery mode cavity[48]; (b) its enhanced version[49].
    Schematic of whispering gallery mode cavity formed by fiber taper and polymer wire[51].
    Fig. 9. Schematic of whispering gallery mode cavity formed by fiber taper and polymer wire[51].
    Schematic of whispering gallery mode cavity formed by metal-doped material[52].
    Fig. 10. Schematic of whispering gallery mode cavity formed by metal-doped material[52].
    Schematic[53](a) and experimental setup[53](b) of proposal from Thompson’s group.
    Fig. 11. Schematic[53](a) and experimental setup[53](b) of proposal from Thompson’s group.
    Schematic of proposal from Sankey’s group[54].
    Fig. 12. Schematic of proposal from Sankey’s group[54].
    Schematic of vibrating membrane cavity with two pumps[55].
    Fig. 13. Schematic of vibrating membrane cavity with two pumps[55].
    Structure of zipper-like photonic crystal cavity[57]
    Fig. 14. Structure of zipper-like photonic crystal cavity[57]
    Structures of (a) snowflake photonic crystal cavity[58], (b) diamond NV center photonic crystal cavity[59], and (c) hexagonal photonic crystal cavity[61].
    Fig. 15. Structures of (a) snowflake photonic crystal cavity[58], (b) diamond NV center photonic crystal cavity[59], and (c) hexagonal photonic crystal cavity[61].
    Structures of (a) distributed superconducting microwave cavity[62] and (b) drum-like superconducting microwave cavity[63].
    Fig. 16. Structures of (a) distributed superconducting microwave cavity[62] and (b) drum-like superconducting microwave cavity[63].
    Schematic (a) and structure (b) of Si3N4 membrane superconducting microwave cavity[64].
    Fig. 17. Schematic (a) and structure (b) of Si3N4 membrane superconducting microwave cavity[64].
    (a) Structure of membrane superconducting microwave cavity designed by Li et al.[65]; (b) experimental setup designed by Bienfait et al.[66].
    Fig. 18. (a) Structure of membrane superconducting microwave cavity designed by Li et al.[65]; (b) experimental setup designed by Bienfait et al.[66].
    (a) Structure of quadrature hybrid coupler[73]; (b) structure of 20 dB directional coupler[73]; (c) schematic of microwave EPR state preparation[74].
    Fig. 19. (a) Structure of quadrature hybrid coupler[73]; (b) structure of 20 dB directional coupler[73]; (c) schematic of microwave EPR state preparation[74].
    Schematic of microwave continuous-variable entanglement state preparation proposed by Li et al.[75].
    Fig. 20. Schematic of microwave continuous-variable entanglement state preparation proposed by Li et al.[75].
    Structure of superconducting microwave cavity designed by Palomaki et al.[76].
    Fig. 21. Structure of superconducting microwave cavity designed by Palomaki et al.[76].
    Schematic of microwave squeezed state preparation and microwave-mechanical vibration mode entanglement preparation proposed by Sete et al.[77].
    Fig. 22. Schematic of microwave squeezed state preparation and microwave-mechanical vibration mode entanglement preparation proposed by Sete et al.[77].
    Schematic of preparing highly squeezed state in microwave domain[78].
    Fig. 23. Schematic of preparing highly squeezed state in microwave domain[78].
    Schematic of cavity electro-opto-mechanical system[79].
    Fig. 24. Schematic of cavity electro-opto-mechanical system[79].
    Schematic of cavity electro-opto-mechanical hybrid quantum interface proposed by Tian[83].
    Fig. 25. Schematic of cavity electro-opto-mechanical hybrid quantum interface proposed by Tian[83].
    Schematic and structure of cavity electro-opto-mechanical converter designed by Andrews et al.[84].
    Fig. 26. Schematic and structure of cavity electro-opto-mechanical converter designed by Andrews et al.[84].
    Schematic of distant microwave fields entanglement preparation proposed by Abdi et al.[85].
    Fig. 27. Schematic of distant microwave fields entanglement preparation proposed by Abdi et al.[85].
    Schematic of microwave quantum illumination based on double cavity electro-opto-mechanical converters[79]
    Fig. 28. Schematic of microwave quantum illumination based on double cavity electro-opto-mechanical converters[79]
    Schematic of Gaussian and non-Gaussian microwave quantum states preparation based on cavity electro-opto-mechanical converter[86].
    Fig. 29. Schematic of Gaussian and non-Gaussian microwave quantum states preparation based on cavity electro-opto-mechanical converter[86].
    Schematic of cavity electro-opto-mechanical converter introducing optical parametric amplifier[87].
    Fig. 30. Schematic of cavity electro-opto-mechanical converter introducing optical parametric amplifier[87].
    Schematic of quantum state transferring proposed by Regal’sgroup[88].
    Fig. 31. Schematic of quantum state transferring proposed by Regal’sgroup[88].
    Schematic of multichannel quantum router based on cavity electro-opto-mechanical[89].
    Fig. 32. Schematic of multichannel quantum router based on cavity electro-opto-mechanical[89].
    Schematic of heraldedmicrowave-optical entanglement preparation based on cavity electro-opto-mechanical system[90].
    Fig. 33. Schematic of heraldedmicrowave-optical entanglement preparation based on cavity electro-opto-mechanical system[90].
    类别品质因数水平振子质量水平振子频率水平优势不足
    法布里-珀罗腔104kg—pgkHz—MHz技术成熟, 应用广泛品质因数水平较低, 耗散较大、不易集成
    回音壁腔109(微球腔) 108(微环腔) ng—fgMHz—GHz光力耦合度高, 构造灵活, 腔内光子寿命长 工艺要求高、成本高
    振动薄膜腔105pgMHz结构简单、灵活耗散较大、不易集成
    光子晶体腔106fgGHz可利用自由度多, 片上可扩展 性好, 精确的模式控制 工艺复杂
    超导微波腔107pgMHz可高度集成, 与超导器件兼容, 腔的稳定性好, 热噪声水平低 超低温, 电磁噪声谱较宽
    Table 1.

    Summary for current research states of 5 main cavity optomechanical systems.

    5种主要腔光力系统的研究现状总结

    腔光力系统类型作用类型模式数腔类型制备的微波非经典量子态
    腔电力系统光子-声子2微波腔连续变量微波纠缠态, 微波压缩态, 微波-机械 振子谐振模纠缠态
    腔电光力系统光子-声子-光子3微波腔, 光腔连续、离散变量微波纠缠态, 微波单光子Fock态, 微波-机械振子谐振模纠缠态, 微波-光纠缠态
    Table 2.

    Preparations of non-classical quantum statesof microwave based on cavity opto-mechanical system

    基于腔光力系统的微波非经典量子态制备

    Jun-Wen Luo, De-Wei Wu, Qiang Miao, Tian-Li Wei. Research progress in non-classical microwave states preparation based on cavity optomechanical system[J]. Acta Physica Sinica, 2020, 69(5): 054203-1
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