• Infrared and Laser Engineering
  • Vol. 51, Issue 5, 20210315 (2022)
Zhiyong Yang, Junchen Song*, Wei Cai, Gaoxiang Lu, and Lina Luo
Author Affiliations
  • Armament Launch Theory and Technology Key Discipline Laboratory of PRC, Rocket Force University of Engineering, Xi′an 710025, China
  • show less
    DOI: 10.3788/IRLA20210315 Cite this Article
    Zhiyong Yang, Junchen Song, Wei Cai, Gaoxiang Lu, Lina Luo. Analysis of polarization-maintaining fibers in non-line-of-sight azimuth transmission system[J]. Infrared and Laser Engineering, 2022, 51(5): 20210315 Copy Citation Text show less

    Abstract

    According to the design requirements of the birefringence of polarization-maintaining fiber in the non-line-of-sight azimuth transmission system, the influence of different types of polarization-maintaining fiber parameters on the birefringence is emphatically analyzed. Firstly, the stress-optical coupling relationship of polarization-maintaining fiber was deduced based on the stress-strain, variational principle and the stress-photoelastic effect. Then, the influence of different factors on the birefringence of polarization-maintaining fiber was investigated by means of finite element analysis software, and two kinds of polarization-maintaining fiber (Panda polarization-maintaining fiber and Bow-tie polarization-maintaining fiber) were compared and analyzed. The results show that the higher birefringence value near the center of the core can be obtained by a variety of methods, such as reducing the distance between the core and the stress zone, increasing cladding radius when fixing core size, or increasing the reference temperature of the polarization-maintaining fiber. Simultaneously, the birefringence of the bow-tie polarization-maintaining fiber is larger in the same conditions. The research results can provide some reference for the design and selection of polarization-maintaining fiber in the non-line-of-sight azimuth transmission system.
    $F = \frac{{\rm{1}}}{{\rm{2}}}\iint_\Omega {{{{\varepsilon}} ^ * }} \cdot {{T}}{\rm{d}}x{\rm{d}}y$(1)

    View in Article

    ${{T}} = [c]\left( {{{\varepsilon}} - {{{\varepsilon}} _{{0}}}} \right)$(2)

    View in Article

    ${\boldsymbol{\varepsilon}} = {\nabla _\varepsilon }{{u}}$(3)

    View in Article

    $F = \frac{1}{2}\iint_\varOmega {{{\left( {{\nabla _\varepsilon }{{u}}} \right)}^ * }} \cdot \left[ c \right]\left( {{\nabla _\varepsilon }{{u}} - {{{\varepsilon}} _0}} \right){\rm{d}}\varOmega $(4)

    View in Article

    ${{u}} = {\left[ N \right]^{\rm{T}}}{\left\{ {{u}} \right\}_e}$(5)

    View in Article

    $\left[ K \right]\left\{ {{u}} \right\} = \left\{ {{f}} \right\}$(6)

    View in Article

    ${{T}} = \left[ c \right]\left( {{{\left[ B \right]}^{\rm{T}}}{{\left\{ {{u}} \right\}}_e} - {{\bf{\varepsilon}} _0}} \right)$(7)

    View in Article

    $\Delta {n_{ij}} = {B_{ijkl}} \cdot {S_{kl}}$(8)

    View in Article

    $\left[ {ΔnxΔnyΔnz} \right] = \left[ {B2B1B1B1B2B1B1B1B2} \right]\left[ {SxSySz} \right]$(9)

    View in Article

    $nx=n0+B2Sx+B1(Sy+Sz)ny=n0+B2Sy+B1(Sx+Sz)nz=n0+B2Sz+B1(Sx+Sy)$(10)

    View in Article

    $nxny=c(SxSy)nynz=c(SySz)nznx=c(SzSy)$(11)

    View in Article

    Zhiyong Yang, Junchen Song, Wei Cai, Gaoxiang Lu, Lina Luo. Analysis of polarization-maintaining fibers in non-line-of-sight azimuth transmission system[J]. Infrared and Laser Engineering, 2022, 51(5): 20210315
    Download Citation