• Photonics Research
  • Vol. 11, Issue 10, 1627 (2023)
Alireza Fardoost1,*, Fatemeh Ghaedi Vanani1, Sethumadhavan Chandrasekhar2, and Guifang Li1,3
Author Affiliations
  • 1CREOL, The College of Optics and Photonics, University of Central Florida, Orlando, Florida 32816, USA
  • 2Retired Nokia Bell Labs, Murray Hill, New Jersey 07974, USA
  • 3e-mail: li@ucf.edu
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    DOI: 10.1364/PRJ.491967 Cite this Article Set citation alerts
    Alireza Fardoost, Fatemeh Ghaedi Vanani, Sethumadhavan Chandrasekhar, Guifang Li, "Single-ended characterization of the coherent transfer matrix of coupled multimode transmission channels," Photonics Res. 11, 1627 (2023) Copy Citation Text show less

    Abstract

    Light propagation in random media is a subject of interest to the optics community at large, with applications ranging from imaging to communication and sensing. However, real-time characterization of wavefront distortion in random media remains a major challenge. Compounding the difficulties, for many applications such as imaging (e.g., endoscopy) and focusing through random media, we only have single-ended access. In this work, we propose to represent wavefronts as superpositions of spatial modes. Within this framework, random media can be represented as a coupled multimode transmission channel. Once the distributed coherent transfer matrix of the channel is characterized, wavefront distortions along the path can be obtained. Fortunately, backreflections almost always accompany mode coupling and wavefront distortions. Therefore, we further propose to utilize backreflections to perform single-ended characterization of the coherent transfer matrix. We first develop the general framework for single-ended characterization of the coherent transfer matrix of coupled multimode transmission channels. Then, we apply this framework to the case of a two-mode channel, a single-mode fiber, which supports two randomly coupled polarization modes, to provide a proof-of-concept demonstration. Furthermore, as one of the main applications of coherent channel estimation, a polarization imaging system through single-mode fibers is implemented. We envision that the proposed method can be applied to both guided and free-space channels with a multitude of applications.
    H=n=1NHn,

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    Ein(x,y,z,t)=E0e^in(x,y)cos[β(zvpt)]e12αz,

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    P*(x,y,z,t)=ε0Δχ(x,y,z)Ein(x,y,z,t).

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    dp=P*dVs=[ε0E0e^in(x,y)Δχ(x,y,zs)e12αzsdVs]dp^cosβ(zvpt).

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    |Es|e^s(x,y)e^in(x,y)Δχ(x,y,zs).

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    Es=0.

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    Er1Er1=H1TRH1Ein1Ein1H1RH1T=H1RH1Ein1Ein1H1RH1,

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    R=r×I=[r00r].

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    Hn=[1+δ11δ12δ211+δ22]n,|δij|1,δijδkh0.

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    |r|2pulse=xr=2Im{Exr1Eyr1*}Im{Exin1Eyin1*}(|Eyin1|2|Exin1|2)|Exr1|2+2Re{Exin1Eyin1*}Re{Exr1Eyr1*}(|Eyin1|2|Exin1|2)|Exin1|2+2Re{Exin1Eyin1*}Re{Exin1Eyin1*}+2Im{Exin1Eyin1*}Im{Exin1Eyin1*},Im{δ11}=Re{Exr1Eyr1*}xrRe{Exin1Eyin1*}4xrIm{Exin1Eyin1*},Im{δ12}=|Exr1|2xr|Exin1|24xrIm{Eyin1Exin1*}.

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    ErnErn=(i=1nHi)R(i=n1Hi)Ein1Ein1(i=1nHi)R(i=n1Hi),

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    Eout_1=H×EinandEout_2=H1×ErN.

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    ρerr=ρ1ρ2ρ2×100%andΨerr=Ψ1Ψ2.

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    POL=III+I

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    H1×[ExEyφ],

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    Alireza Fardoost, Fatemeh Ghaedi Vanani, Sethumadhavan Chandrasekhar, Guifang Li, "Single-ended characterization of the coherent transfer matrix of coupled multimode transmission channels," Photonics Res. 11, 1627 (2023)
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