基于双核心的软玻璃 photonic 水晶,纤维(PCF ) 用微米规模金牌电线填满的极化 splitter 被建议。极化 splitter 的特征被与有限元素方法改变 PCF 和金电线的直径的结构的参数学习(女性) 。模拟结果表明软基于眼镜的 PCF 的联合长度比率接近 2,相应曲线比基于硅石的 PCF 的完全是更多。宽带带宽是扑灭比率是比由软基于眼镜的 PCF 的 20 dB 低的 226 在 nm,即,从 1465,到在报导极化 splitters 竞争的 1691 nm 的 nm,和带宽只是由基于硅石的 PCF 的 32 nm。由我们的极化 splitter 的插入损失只在 1.47 m 和 1.55 m 的波长是 0.00248 dB 和 0.43 dB。birefringence 显然被增加,联合长度被充满金电线进减少软基于眼镜或基于硅石的 PCF。另外 birefringence 基于金电线被介绍的软基于眼镜的 PCF 基于基于硅石的 PCF 比那大得多。极化 splitter 的制造忍耐被改变结构的参数也考虑。极化 splitter 拥有宽广带宽,低插入损失,简单结构和高制造忍耐。
A polarization splitter based on dual-core soft glass photonic crystal fiber (PCF) filled with micron-scale gold wire is proposed. The characteristics of the polarization splitter are studied by changing the structural parameters of the PCF and the diameter of the gold wire with the finite element method (FEM). The simulation results reveal that the coupling length ratio of the soft glass-based PCF is close to 2 and the corresponding curve is more fiat than that of the silica-based PCE The broadband bandwidth is 226 nm in which the extinction ratio is lower than -20 dB by the soft glass-based PCE i.e., from 1465 nm to 1691 nm which is competitive in the reported polarization splitters, and the bandwidth is just 32 nm by the silica-based PCE The insertion loss by our polarization splitter is just 0.00248 dB and 0.43 dB at the wavelength of 1.47 μm and 1.55 μm. The birefringence is obviously increased and the coupling length is decreased by filling gold wire into the soft glass-based or the silica-based PCE Also the birefringence based on the silica-based PCF is much larger than that based on the soft glass-based PCF whether or not the gold wire is introduced. The fabrication tolerance of the polarization splitter is also considered by changing the structural parameters. The polarization splitter possesses broad bandwidth, low insertion loss, simple structure and high fabrication tolerance.