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Coupled-Mode Analysis for Chiral Fiber Long-Period Gratings Using Local Mode Approach

机译:使用局部模式方法的手性光纤长周期光栅耦合模式分析

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Starting from the conventional coupled-mode theory and using the mode transformation method, a unified local mode approach is presented to analyze the chiral fiber long-period gratings (CLPGs) formed by twisting a high-birefringence fiber as an example of a chiral fiber with double-helix symmetry. Similarly, a helical-core fiber, as an example of single-helix CLPGs, is analyzed by using the ideal mode approach. The coupled-mode equations for both the cases are transformed and reduced to two-mode equations. The derivation is simple, and the results are explicit in concept. These results reveal the scheme of polarization selectivity of mode coupling, and for the first time, the necessary condition for achieving the polarization selection is given. The analysis indicates that conventional coupled-mode theory is efficient for studying chiral fiber grating, and more importantly, it is better to be understood. A numerical simulation has been done on a twisted conventional Panda fiber with a beat length of 2.5 mm. It has been shown that in a right-handed twisted structure, a total power transfer of a right-handed circular polarization light is obtained with a grating pitch of 0.382 mm and a grating length of 64.9 mm at the wavelength of 1.55 μm . On the other hand, through the simulation on single-helix CLPG with an eccentric core, it has been shown that a total power transfer of the core mode to LP11 mode is obtained with a grating pitch of 0.723 mm and a grating length of 10.46 mm at the wavelength of 1.55 μm.
机译:从传统的耦合模式理论出发,并采用模式转换方法,提出了一种统一的局部模式方法来分析通过扭曲高双折射光纤形成的手性光纤长周期光栅(CLPG),例如双螺旋对称。类似地,通过使用理想模式方法来分析螺旋芯光纤(作为单螺旋CLPG的示例)。两种情况下的耦合模方程均被转换并简化为双模方程。推导很简单,并且结果在概念上是明确的。这些结果揭示了模式耦合的极化选择性方案,并且首次给出了实现极化选择的必要条件。分析表明,传统的耦合模式理论对于研究手性光纤光栅是有效的,更重要的是,它易于理解。已对节拍长度为2.5 mm的传统双绞加捻光纤进行了数值模拟。已经表明,在右旋扭曲结构中,在1.55μm的波长下以0.382mm的光栅间距和64.9mm的光栅长度获得右旋圆偏振光的总功率传递。另一方面,通过对带有偏心磁芯的单螺旋CLPG进行仿真,结果表明,在0.723 mm的光栅间距和10.46 mm的光栅长度下,可以获得从芯模式到LP11模式的总功率传输。在1.55μm的波长下

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