• Laser & Optoelectronics Progress
  • Vol. 60, Issue 9, 0900001 (2023)
Yunqi Liu1、*, Chen Jiang1, Zuyao Liu1、2, and Xinyi Zhao1、3
Author Affiliations
  • 1Key Laboratory of Specialty Fiber Optics and Optical Access Networks, Ministry of Education, School of Communication and Information Engineering, Shanghai University, Shanghai 200444, China
  • 2Key Laboratory of Optoelectronic and Telecommunication of Jiangxi Province, School of Physics and Communication Electronics, Jiangxi Normal University, Nanchang 330022, Jiangxi, China
  • 3Henan Key Laboratory of Optoelectronic Sensing Integrated Application, College of Electronic and Electrical Engineering, Henan Normal University, Xinxiang 453007, Henan, China
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    DOI: 10.3788/LOP220735 Cite this Article Set citation alerts
    Yunqi Liu, Chen Jiang, Zuyao Liu, Xinyi Zhao. Long-Period Fiber Gratings[J]. Laser & Optoelectronics Progress, 2023, 60(9): 0900001 Copy Citation Text show less

    Abstract

    As an important passive optical component, long-period fiber gratings (LPFGs) have all the advantages of optical fiber sensors, such as anti-electromagnetic interference, corrosion resistance, high sensitivity, small volume, and compatible with fiber system, which have wide applications in the field of optical fiber sensors and optical communications. The paper summarizes the principle of mode coupling, the methods of theoretical analysis, fabrication techniques, and applications of the LPFGs in the field of optical fiber sensors and optical communications. The fabrication techniques include the laser inscribing techniques (UV laser, carbon dioxide laser, and femtosecond laser writing techniques) and non-laser techniques (arc discharge, mechanical micro-bending, cladding etching, fusion tapering, ion implantation, and acoustic wave modulation techniques). For the sensing application of the LPFGs, the characteristics of gratings on the temperature, strain, bending, torsion, and surrounding refractive index have been summarized. And their applications as all fiber filter, mode convertor, polarizer, and mode coupler have also been discussed for the applications in optical communication system. The paper is written in a tutorial style. We aim to provide a general reference for students, academics who are going to join in this field.
    λ=neff01-neffnmΛ/N
    ×E=-Bt×H=Dt D=0 B=0
    2E+k2E=02H+k2H=0
    Ex,y,z=e(x,y)exp-iβzHx,y,z=hx,yexp-iβz
    t2+k2-β2e=0t2+k2-β2h=0
    EHx,y,z=iaieibihix,yexp-iβiz
    HE1nLP0nHE2n+TE0nLP1nHE2n+TM0nLP1nHEm+1,n+EHm-1,nLPmn(m2,n1)
    hx(r,ϕ)=-ωεβa0JmUa1rexpjmϕ   , 0ra1b0KmWa1rexpjmϕ  ,  r>a1
    ez(r,ϕ)=a0jβexpjmϕUsinϕa1Jm'Ura1+jmcosϕrJmUra1  ,    0ra1b0jβexpjmϕWsinϕa1Km'Wra1+jmcosϕrKmWra1 ,   r>a1
    hz(r,ϕ)=a0-jωμ0expjmϕUcosϕa1Jm'Ura1-jmsinϕrJmUra1   ,   0ra1b0-jωμ0expjmϕWcosϕa1Km'Wra1-jmsinϕrKmWra1  ,  r>a1
    nco(z)=n1+δn(z)
    δn(z)=Δnrect(z/Λ)
    rect(z /Λ)=1,nΛ  z  nΛ+pΛ0,nΛ+pΛ< z  (n+1)Λ,(n=0, 1, 2, , N; 0 < p <1)
    dAcodz=iκ11-11co-coAco+i2vκ1v-11cl-coAvcl×m=1+Amexp(-i2δ1v-11cl-coz)vdAvcldz+iκ1v-11cl-coAco×m=1+Amexp(-i2δ1v-11cl-coz),
    k11-11co-co(z)=ωε0n12σ(z)202πdϕ0a1rdrErco2+Eϕco2
    k1v-11cl-co(z)=ωε0n12σ(z)202πdϕ0a1rdr(ErclErco*+EϕclEϕco*)
    δ1v-11cl-co=12β11co-β1vcl-2πΛ
    T(λ)=A(L)2=cos2σ^2+κ2L+11+κ2/σ^2sin2σ^2+κ2L
    λ=neff01-neff,clnmΛ
    dλ/dT=λγ(α+Γtemp)
    dλ/dε=λγ(1+Γstrain)
    dλ/dnsur=λγΓsur
    γ=(dλ/dΛ)/(neff01-neff,clnm)
    Γtemp=ξconeff01 - ξclneff,clnmncoeff- neff,clnm
    Γstrain=ηconeff01 - ηclneff,clnmneff01- neff,clnm
    Γsur=-um2λres3nsur8πrcl3ncl(neff01- neff,clnm)(ncl2 - nsur3)3/2
    Δλm=(neff01-neff,clnm)ΔΛ+ΔnΔΛ
    Δn=cσ
    Δλ(m)-δneff,clnmΛ
    E˙=GR˙T
    Δλm=(neff01-neff,clnm)ΔΛ-δneff,clnmΛ
    To=Tcl2-2TcoTclcos(φ+δ)
    Tcl=1-Tco
    φ=2πΔneff,clnmLλm
    RFSR=λ2Δneff,clnmL
    Yunqi Liu, Chen Jiang, Zuyao Liu, Xinyi Zhao. Long-Period Fiber Gratings[J]. Laser & Optoelectronics Progress, 2023, 60(9): 0900001
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