• Journal of Infrared and Millimeter Waves
  • Vol. 39, Issue 6, 696 (2020)
Ying HAN1、*, Zheng-Ran LI1, Wei-Zhen ZHU1, Peng SONG2, Fan-Di ZHOU1, Qi-Hao YANG1, Yan WANG1, Lin GONG1, Man YANG1, Wei WANG1, and Lan-Tian HOU1
Author Affiliations
  • 1The Key Laboratory for Special Fiber and Fiber Sensor of Hebei Province, Institute of Information Science and Technology, Yanshan University, Qinhuangdao066004, China
  • 2School of Physics and Technology, University of Jinan, Jinan250022, China
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    DOI: 10.11972/j.issn.1001-9014.2020.06.006 Cite this Article
    Ying HAN, Zheng-Ran LI, Wei-Zhen ZHU, Peng SONG, Fan-Di ZHOU, Qi-Hao YANG, Yan WANG, Lin GONG, Man YANG, Wei WANG, Lan-Tian HOU. Polarization-maintaining hollow core negative curvature fiber with an operating wavelength of 2.94 μm[J]. Journal of Infrared and Millimeter Waves, 2020, 39(6): 696 Copy Citation Text show less
    Polarization maintain hollow core negative curvature fiber end view
    Fig. 1. Polarization maintain hollow core negative curvature fiber end view
    (a)y-directional clad tube thickness t1y and nested tube to the inner diameter of the tube maximum distance Z on the influence of HC-NCF PER ,(b)when t1y/t1xis 2.15 (t1y is 1.60 μm), Z is 11.76 μm, x and y direction polarization mode
    Fig. 2. (a)y-directional clad tube thickness t1y and nested tube to the inner diameter of the tube maximum distance Z on the influence of HC-NCF PER ,(b)when t1y/t1xis 2.15 (t1y is 1.60 μm), Z is 11.76 μm, x and y direction polarization mode
    The effect of core diameter Dcore on polarization maintain HC-PCF (a) The confinement loss of the modes changes with Dcore, (b) PER and HOMER changes with Dcore, (c) Re(neff) change with Dcore,(d) the mode-field coupling process
    Fig. 3. The effect of core diameter Dcore on polarization maintain HC-PCF (a) The confinement loss of the modes changes with Dcore, (b) PER and HOMER changes with Dcore, (c) Re(neff) change with Dcore,(d) the mode-field coupling process
    The effect of the cladding tube diameter Dtube on polarization maintain HC-NCF (a) the confinement loss of the mode changes with Dtube, (b) Re(neff) changes with Dtube
    Fig. 4. The effect of the cladding tube diameter Dtube on polarization maintain HC-NCF (a) the confinement loss of the mode changes with Dtube, (b) Re(neff) changes with Dtube
    Coupling process of mode changing with Dtube: When Dtube=79.57 μm, (a) x-pol core mode, (b) Clad surface mode1; When Dtube=91.14μm, (c) y-pol core mode, (d) Clad surface mode2
    Fig. 5. Coupling process of mode changing with Dtube: When Dtube=79.57 μm, (a) x-pol core mode, (b) Clad surface mode1; When Dtube=91.14μm, (c) y-pol core mode, (d) Clad surface mode2
    Polarization maintain HC-NCF mode coupling process with wavelength change (a) effective refractive index, (b)coupling process of mode
    Fig. 6. Polarization maintain HC-NCF mode coupling process with wavelength change (a) effective refractive index, (b)coupling process of mode
    Polarization maintain HC-NCF transmission characteristics with wavelength change (a) Mode-limited loss changes with wavelength, (b) PER and HOMER change with wavelength, (c) Birefringence change with wavelength, (d) x-pol core mode(top) and high order mode(bottom)
    Fig. 7. Polarization maintain HC-NCF transmission characteristics with wavelength change (a) Mode-limited loss changes with wavelength, (b) PER and HOMER change with wavelength, (c) Birefringence change with wavelength, (d) x-pol core mode(top) and high order mode(bottom)
    Bend loss of polarization-maintaining HC-NCF (a) the loss obtained by bend in the y direction, (b) the loss obtained by bend in the x direction
    Fig. 8. Bend loss of polarization-maintaining HC-NCF (a) the loss obtained by bend in the y direction, (b) the loss obtained by bend in the x direction
    Ying HAN, Zheng-Ran LI, Wei-Zhen ZHU, Peng SONG, Fan-Di ZHOU, Qi-Hao YANG, Yan WANG, Lin GONG, Man YANG, Wei WANG, Lan-Tian HOU. Polarization-maintaining hollow core negative curvature fiber with an operating wavelength of 2.94 μm[J]. Journal of Infrared and Millimeter Waves, 2020, 39(6): 696
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