• Photonics Research
  • Vol. 12, Issue 3, 411 (2024)
Darcy L. Smith1、2、3、4、†,*, Linh V. Nguyen3、4、†, Mohammad I. Reja1、3, Erik P. Schartner1, Heike Ebendorff-Heidepriem1, David J. Ottaway1、2, and Stephen C. Warren-Smith3、4
Author Affiliations
  • 1Institute for Photonics and Advanced Sensing and School of Physics, Chemistry and Earth Sciences, The University of Adelaide, Adelaide, SA 5005, Australia
  • 2Australian Research Council Centre of Excellence for Gravitational Wave Discovery (OzGrav), Adelaide, SA, Australia
  • 3Future Industries Institute, University of South Australia, Mawson Lakes, SA 5095, Australia
  • 4Laser Physics and Photonics Devices Laboratory, University of South Australia, Mawson Lakes, SA 5095, Australia
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    DOI: 10.1364/PRJ.507542 Cite this Article Set citation alerts
    Darcy L. Smith, Linh V. Nguyen, Mohammad I. Reja, Erik P. Schartner, Heike Ebendorff-Heidepriem, David J. Ottaway, Stephen C. Warren-Smith. Harnessing the power of complex light propagation in multimode fibers for spatially resolved sensing[J]. Photonics Research, 2024, 12(3): 411 Copy Citation Text show less

    Abstract

    The propagation of coherent light in multimode optical fibers results in a speckled output that is both complex and sensitive to environmental effects. These properties can be a powerful tool for sensing, as small perturbations lead to significant changes in the output of the fiber. However, the mechanism to encode spatially resolved sensing information into the speckle pattern and the ability to extract this information are thus far unclear. In this paper, we demonstrate that spatially dependent mode coupling is crucial to achieving spatially resolved measurements. We leverage machine learning to quantitatively extract the spatially resolved sensing information from three fiber types with dramatically different characteristics and demonstrate that the fiber with the highest degree of spatially dependent mode coupling provides the greatest accuracy.
    E(x,y,z)=j=1NAj(z)e^j(x,y),

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    A=(A1(z),,AN(z)).

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    A(out)=M(t)A(in),

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    M(k)=V(k)Λ(k)U(k)*,

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    Λ(k)=[exp(12g1(k)iϕ1(k))00exp(12gN(k)iϕN(k))],

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    M(t)=M(K)M(K1)M(k)M(2)M(1).

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    Λ˜=[exp(iΔϕ1)00exp(iΔϕN)].

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    M(t)=M(K)M(K1)V(k)Λ˜Λ(k)U(k)*M(2)M(1).

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    Z[I(λ)]=λ[I0(λ)I¯0][I(λ)I¯]{λ[I0(λ)I¯0]2λ[I(λ)I¯]2}12,

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    Darcy L. Smith, Linh V. Nguyen, Mohammad I. Reja, Erik P. Schartner, Heike Ebendorff-Heidepriem, David J. Ottaway, Stephen C. Warren-Smith. Harnessing the power of complex light propagation in multimode fibers for spatially resolved sensing[J]. Photonics Research, 2024, 12(3): 411
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