• Photonics Research
  • Vol. 7, Issue 10, 1142 (2019)
Qian Zhao, Zhong-Jian Yang*, and Jun He
Author Affiliations
  • Hunan Key Laboratory of Super Microstructure and Ultrafast Process, School of Physics and Electronics, Central South University, Changsha 410083, China
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    DOI: 10.1364/PRJ.7.001142 Cite this Article Set citation alerts
    Qian Zhao, Zhong-Jian Yang, Jun He, "Coherent couplings between magnetic dipole transitions of quantum emitters and dielectric nanostructures," Photonics Res. 7, 1142 (2019) Copy Citation Text show less

    Abstract

    Here we study theoretically the optical responses of hybrid structures composed of dielectric nanostructures and quantum emitters with magnetic dipole transitions. Coherent couplings between magnetic dipole transitions and magnetic modes can occur, leading to giant modifications of the extinction spectra of the constituents in the hybrid structures. For a given hybrid structure, the extinction-cross-section spectra show linear or nonlinear behaviors depending on the strength of the excitation field. For a weak excitation, the extinction of the quantum emitters is greatly enhanced. The hybrid structure shows a dip on its extinction spectrum. For a strong excitation, the resonant extinction of the quantum emitters is weakly enhanced while the extinction spectrum is broadened obviously. The hybrid structure shows a Fano-like line shape on its extinction spectrum, which is different from that with a weak excitation. This difference is highly related to the behaviors of the magnetic polarizabilities of the quantum emitters in the hybrid structure. The optical responses of hybrid structures can be largely tuned by varying the geometric and material parameters.
    H^MD=ω0a^a^μMDBMDa^μMDBMD*a^.(1)

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    BMD(t)=μMD[(Ω+Gρ¯21)eiωt+(Ω*+G*ρ¯12)eiωt],=(BMD/2)eiωt+(BMD*/2)eiωt(2)

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    dρijdt=i[ρ,HMD]ijΓijρij,(3)

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    dρ21dt=iω0ρ21+iμMDBMD(t)(ρ11ρ22)ρ21T2,d(ρ11ρ22)dt=2iμMDBMD(t)(ρ21ρ21*)(ρ11ρ22)(ρ11ρ22)0T1,(4)

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    dCdt=CT2+(ωω0)D(ΩI+GICGRD)Δ,dDdt=DT2(ωω0)C(ΩR+GRCGID)Δ,dΔdt=1ΔT1+4ΩIC+4ΩRD+4GI(C2+D2),(5)

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    αMD=Nμ0μMD2(ω0ω)T22+T2i1+(ωω0)2T22+μMD22|BMD|2T1T2.(6)

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    (σext)MD=kNμ0μMD2T21+(ωω0)2T22+μMD22|BMD|2T1T2|BMD|2B02.(7)

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    Δω=2T22|BMD1|2|BMD0|21+μMD22|BMD1|2T1T2,(8)

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    (σext)Si=μ0kIm(mSiBSi*)B02+kIm(αE)=kIm(αM){[B0+Re(YmMD)]2+[Im(YmMD)]2}B02+kIm(αE).(9)

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    (σext)MD1(kNT2μ0μMD2|BMD0|2)/(B02),(10)

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    Δω(2/T2)2|BMD1|2/|BMD0|21.(11)

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    (σext)MD2kNμ0/(B02T1).(12)

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    Δω2μMD|BMD1|T1T2/(T2).(13)

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    Qian Zhao, Zhong-Jian Yang, Jun He, "Coherent couplings between magnetic dipole transitions of quantum emitters and dielectric nanostructures," Photonics Res. 7, 1142 (2019)
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