• Photonics Research
  • Vol. 11, Issue 5, 852 (2023)
Mingsheng Tian1、†, Fengxiao Sun1、†, Kaiye Shi2, Haitan Xu3、4、5、9、*, Qiongyi He1、6、7、10、*, and Wei Zhang2、8、11、*
Author Affiliations
  • 1State Key Laboratory for Mesoscopic Physics, School of Physics, Frontiers Science Center for Nano-optoelectronics, and Collaborative Innovation Center of Quantum Matter, Peking University, Beijing 100871, China
  • 2Department of Physics, Renmin University of China, Beijing 100872, China
  • 3School of Materials Science and Intelligent Engineering, Nanjing University, Suzhou 215163, China
  • 4Shishan Laboratory, Nanjing University, Suzhou 215163, China
  • 5School of Physical Sciences, University of Science and Technology of China, Hefei 230026, China
  • 6Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, China
  • 7Hefei National Laboratory, Hefei 230088, China
  • 8Beijing Academy of Quantum Information Sciences, Beijing 100193, China
  • 9e-mail: haitanxu@nju.edu.cn
  • 10e-mail: qiongyihe@pku.edu.cn
  • 11e-mail: wzhangl@ruc.edu.cn
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    DOI: 10.1364/PRJ.485595 Cite this Article Set citation alerts
    Mingsheng Tian, Fengxiao Sun, Kaiye Shi, Haitan Xu, Qiongyi He, Wei Zhang. Nonreciprocal amplification transition in a topological photonic network[J]. Photonics Research, 2023, 11(5): 852 Copy Citation Text show less

    Abstract

    We studied the transport properties of a driven-dissipative photonic network, where multiple photonic cavities are coupled through a nonreciprocal bus with unidirectional transmission. For short-range coupling between the cavities, the occurrence of nonreciprocal amplification can be linked to a topological phase transition of the underlying dynamic Hamiltonian. However, for long-range coupling, we show that the correspondence between the nonreciprocal amplification transition and the topological phase transition breaks down as the transition conditions deviate significantly from each other. We found the exact transition condition for nonreciprocal amplification, supported by analytical calculation and numerical simulation. We also investigated the stability, the crossover from short- to long-range coupling, and the bandwidth of the nonreciprocal amplification. Our work has potential applications in signal transmission and amplification, and also paves the way to study other topological and non-Hermitian systems with long-range coupling and nontrivial boundary effects.
    a^˙j(t)=γjκjΓ2iω02a^j(t)κja^j,in(t)l<jNΓjleikωxjla^l(t)=iω0aj(t)+l=1jHjla^l(t)κja^j,in(t),

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    aout(ω)={I+κ[H+i(ωω0)I]1}ain(ω)=S(ω)ain(ω),

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    |Sjl|={|γ+κΓ+2iΔωγκΓ+2iΔω|,for      j=l;0,for      j<l;Be(jl)(ξ1ζ1),for    j>l.

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    B=4κΓ|(γ+Γκ+2iΔω)(γΓκ+2iΔω)|,ξ=(ln|γ+Γκ+2iΔωγΓκ+2iΔω|)1,

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    γ>κ+Γ2Γe1/ζ+1

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    hp(k)=m=0N1μmeikm,

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    νp=12πi02πdkhp(k)hp(k)=12πi02πdkddkloghp(k).

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    Mp=j=1Nm=0N1μm|j+mj|=1Nj=1Nm=0N1μmkeik(m+j)keikj|kk|=km=0N1μmeikm|kk|=khp(k)|kk|,(A1)

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    hp(k)=γκΓ2+iΔωΓei(kωk)1/ζeiN(kωk)N/ζ1ei(kωk)1/ζ,(A2)

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    γ=κ+Γ+2Γei(kωk)1/ζeiN(kωk)N/ζ1ei(kωk)1/ζ2iΔω.(A3)

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    γ=κ+Γ2Γe1/ζ+1.(A4)

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    hp(k)=γκΓ2+iΔωΓei(kωk)eiN(kωk)1ei(kωk).(A5)

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    γ=κΓ,(A6)

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    Mingsheng Tian, Fengxiao Sun, Kaiye Shi, Haitan Xu, Qiongyi He, Wei Zhang. Nonreciprocal amplification transition in a topological photonic network[J]. Photonics Research, 2023, 11(5): 852
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