• Photonics Research
  • Vol. 8, Issue 9, B8 (2020)
Luqi Yuan1、*, Avik Dutt2, Mingpu Qin3, Shanhui Fan2、5, and Xianfeng Chen1、4、6
Author Affiliations
  • 1State Key Laboratory of Advanced Optical Communication Systems and Networks, School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
  • 2Department of Electrical Engineering, and Ginzton Laboratory, Stanford University, Stanford, California 94305, USA
  • 3School of Physics and Astronomy, Shanghai Jiao Tong University, Shanghai 200240, China
  • 4Collaborative Innovation Center of Light Manipulations and Applications, Shandong Normal University, Jinan 250358, China
  • 5e-mail: shanhui@stanford.edu
  • 6e-mail: xfchen@sjtu.edu.cn
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    DOI: 10.1364/PRJ.396731 Cite this Article Set citation alerts
    Luqi Yuan, Avik Dutt, Mingpu Qin, Shanhui Fan, Xianfeng Chen. Creating locally interacting Hamiltonians in the synthetic frequency dimension for photons[J]. Photonics Research, 2020, 8(9): B8 Copy Citation Text show less

    Abstract

    The recent emerging field of synthetic dimension in photonics offers a variety of opportunities for manipulating different internal degrees of freedom of photons such as the spectrum of light. While nonlinear optical effects can be incorporated into these photonic systems with synthetic dimensions, these nonlinear effects typically result in long-range interactions along the frequency axis. Thus, it has been difficult to use the synthetic dimension concept to study a large class of Hamiltonians that involves local interactions. Here we show that a Hamiltonian that is locally interacting along the synthetic dimension can be achieved in a dynamically modulated ring resonator incorporating χ(3) nonlinearity, provided that the group velocity dispersion of the waveguide forming the ring is specifically designed. As a demonstration we numerically implement a Bose–Hubbard model and explore photon blockade effect in the synthetic frequency space. Our work opens new possibilities for studying fundamental many-body physics in the synthetic space in photonics, with potential applications in optical quantum communication and quantum computation.
    HBH=Jm(amam+1+h.c.)g2mamamamam,(1)

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    T=ei2αcos(Ωt),(2)

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    2πΩEmτΔEm=iα(Em+1+Em1),(3)

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    H0=Jm(amam+1+h.c.).(4)

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    H2=Jm(amam+1+h.c.)g2m,n,p,qamanapaqg3m,n(aman3+h.c.),(5)

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    A(z,ω)z=iβ(ω)A(z,ω),(6)

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    β(ω)β(ω0)=dβdω|ω0(ωω0)+12d2βdω2|ω0(ωω0)2+.(7)

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    A(z=L,ω)=A(z=0,ω)eiβ0Li(ωω0)L/vgiβ2(ωω0)2L/2.(8)

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    A˜3z=iω022β0c2χ(3)A˜1A˜2A˜4*eiΔkz,(9)

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    A˜4z=iω022β0c2χ(3)A˜1A˜2A˜3*eiΔkz,(10)

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    Δk=β22[(ω3ω0)2+(ω4ω0)2(ω1ω0)2(ω2ω0)2].(11)

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    2πΩA˜mτ=iα(A˜m+1+A˜m1)+iω022β0c2χ(3)|A˜m|2A˜m+inm2ω02β0c2χ(3)|A˜n|2A˜m,(12)

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    H3=Jm(amam+1+h.c.)g2mamamamamgnmanamaman.(13)

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    nmanamaman=mamam(nmanan)=mamam(Namam)=N2Nmamamamam.(14)

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    H4=Jm(amam+1+h.c.)+g2mamamamamg(N2N).(15)

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    dam(t)dt=i[H3,am]γam(t)+iγcin,m(t),(16)

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    cout,m(t)=cin,m(t)iγam(t),(17)

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    dout,m(t)=iγam(t),(18)

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    |ϕ(p,q)=dt1dt2f(t1+t22)h(t1t2)cin,q(t2)cin,p(t1)|0,(19)

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    Pm,n=dtGm,n(2)(t,t).(20)

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    Luqi Yuan, Avik Dutt, Mingpu Qin, Shanhui Fan, Xianfeng Chen. Creating locally interacting Hamiltonians in the synthetic frequency dimension for photons[J]. Photonics Research, 2020, 8(9): B8
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