Low-Loss and Weakly Coupled Eight-Mode Nodeless Hollow-Core Anti-Resonant Fiber With Three-Layer Nested Tubes in Each Cladding Unit

A low-loss and weakly coupled eight-mode nodeless hollow-core anti-resonant fiber (HC-ARF) is designed and analyzed. The cladding structure comprising six cladding units with three-layer nested tubes suppresses mode coupling between the eight core modes (LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</sub>-LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">31a</sub>, LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">31b</sub>-LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">41</sub>) and cladding modes. By optimizing the core radius and nested tubes, the confinement losses of the LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</sub>-LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">41</sub> modes can be controlled to be below 1.72 × 10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">−4</sup> dB/m. The effective refractive index difference between adjacent core modes is greater than 1.0 × 10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">−4</sup>, and the corresponding differential mode group delay is larger than 0.38 ps/m in the wavelength range between 1480 nm and 1670 nm. As a result, weak coupling can be accomplished between LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</sub>-LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">41</sub>, and these eight core modes can propagate through the HC-ARF with similar low losses. Numerical analysis demonstrates that the eight weakly coupled modes can be stably supported at a bending radius of 20 cm. At smaller bending radii of 5 and 3 cm, five and two weakly coupled core modes, respectively, can still be supported.

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Publication Details

Journal
Journal of Lightwave Technology
Published
2024-11-27
DOI
https://doi.org/10.1109/jlt.2024.3507111
Citations
2
Primary Topic
Optical Network Technologies
Type
article
Field-Weighted Citation Impact
0.42
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article

Low-Loss and Weakly Coupled Eight-Mode Nodeless Hollow-Core Anti-Resonant Fiber With Three-Layer Nested Tubes in Each Cladding Unit

Wei Gao, Paul Kim-Ho Chu, Xin Wang, Biao Wang et al.
2 citations
Journal of Lightwave Technology
Optical Network Technologies
0.42
article

Low-Loss and Weakly Coupled Eight-Mode Nodeless Hollow-Core Anti-Resonant Fiber With Three-Layer Nested Tubes in Each Cladding Unit

Wei Gao, Paul Kim-Ho Chu, Xin Wang, Biao Wang, Lou Shu-Qin
article en
2 citations

Abstract

A low-loss and weakly coupled eight-mode nodeless hollow-core anti-resonant fiber (HC-ARF) is designed and analyzed. The cladding structure comprising six cladding units with three-layer nested tubes suppresses mode coupling between the eight core modes (LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</sub>-LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">31a</sub>, LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">31b</sub>-LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">41</sub>) and cladding modes. By optimizing the core radius and nested tubes, the confinement losses of the LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</sub>-LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">41</sub> modes can be controlled to be below 1.72 × 10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">−4</sup> dB/m. The effective refractive index difference between adjacent core modes is greater than 1.0 × 10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">−4</sup>, and the corresponding differential mode group delay is larger than 0.38 ps/m in the wavelength range between 1480 nm and 1670 nm. As a result, weak coupling can be accomplished between LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">01</sub>-LP<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">41</sub>, and these eight core modes can propagate through the HC-ARF with similar low losses. Numerical analysis demonstrates that the eight weakly coupled modes can be stably supported at a bending radius of 20 cm. At smaller bending radii of 5 and 3 cm, five and two weakly coupled core modes, respectively, can still be supported.

Journal of Lightwave TechnologyVol. 43(6)
City University of Hong Kong (HK), Beijing Jiaotong University (CN), Beijing Municipal Education Commission (CN)
Affordable and clean energy
Openalex Percentile: Top 36%
Optical Network Technologies
0.42
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