Design of a Metal-Filled Photonic-Crystal Fiber Polarization Filter Based on Surface Plasmon Resonance at 1.31 and 1.55&#x00A0;<inline-formula><tex-math notation="LaTeX">$\mu$</tex-math></inline-formula>m

A metal-filled photonic crystal fiber (PCF) polarization filter based on surface plasmon resonance (SPR) is proposed and designed. The structure of the cross-section of a PCF is composed of a hexagonal lattice of air holes, in which an air hole is selectively filled with metal. We realize the polari...

Full description

Saved in:
Bibliographic Details
Main Authors: Xinglian Lu, Min Chang, Nan Chen, Xuedian Zhang, Songlin Zhuang, Jian Xu
Format: Article
Language:English
Published: IEEE 2018-01-01
Series:IEEE Photonics Journal
Subjects:
Online Access:https://ieeexplore.ieee.org/document/8478409/
Tags: Add Tag
No Tags, Be the first to tag this record!
Description
Summary:A metal-filled photonic crystal fiber (PCF) polarization filter based on surface plasmon resonance (SPR) is proposed and designed. The structure of the cross-section of a PCF is composed of a hexagonal lattice of air holes, in which an air hole is selectively filled with metal. We realize the polarization filter at the communication wavelengths of 1.31 and 1.55&#x00A0;<inline-formula><tex-math notation="LaTeX">$\mu$</tex-math></inline-formula>m with optimized structural parameters. The losses of the X polarization mode are 25126.44 and 22444.54&#x00A0;dB&#x002F;m, while the losses of the Y polarization mode are about 1375.81 and 358.62&#x00A0;dB&#x002F;m at the resonance wavelengths 1.31 and 1.55&#x00A0;<inline-formula><tex-math notation="LaTeX">$\mu$</tex-math></inline-formula>m, respectively. Therefore, the two light polarizations can be clearly separated. When the fiber length is 600&#x00A0;<inline-formula> <tex-math notation="LaTeX">$\mu$</tex-math></inline-formula>m, cross-talk is over 20&#x00A0;dB at the communication wavelengths, while the achieved bandwidth is 160 and 200 nm at 1.31 and 1.55&#x00A0;<inline-formula> <tex-math notation="LaTeX">$\mu$</tex-math></inline-formula>m, respectively. Furthermore, the distance between the resonance peaks of the two polarizations can reach 267 nm at 1.55&#x00A0;<inline-formula><tex-math notation="LaTeX"> $\mu$</tex-math></inline-formula>m, achieving a significantly higher value than previously reported. These results are of great significance for the development of a polarization filter applicable in targeted communication bands.
ISSN:1943-0655