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Higher-order dispersion terms of a photonic crystal fiber with hexagonal holes

机译:具有六角孔的光子晶体光纤的高阶色散项

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In the modeling of supercontinuum generation in photonic crystal fibers by ultrashort pulses, the knowledge of the higher-order dispersion terms of the fiber are necessary to achieve a good approximation between the simulated and experimental spectra. However, these parameters are usually not provided by the manufacturer. In this work, we present the numerical estimation of the higher-order dispersion terms for a nonlinear photonic crystal fiber with hexagonal holes. For the simulation, we chose a commercial fiber with a high nonlinear response (Blazephotonics NL-2.4-8). The fiber was designed with a small core diameter of 2.4 μm and a triangular pattern of air holes in the cladding with a pitch of 2.9 μm. Through the free software, MIT Photonic Bands, the structure of the fiber was modeled and the effective refractive index, as well as the dispersion terms curves are estimated. From our results, the zero-dispersion wavelength of the fiber resulted to be of 800 run and at this wavelength, the higher-order dispersion terms were: β_2=0, β_3=0.05 ps~3/km, β_4=-7.03×l0~(-5) ps~4/km, β_5=1.4×10~(-7) ps5/km, β_6=-4.163×10~(-10) ps~6/km, β_7=1.118×10~(-12) ps~7/km. The zero-dispersion wavelength and the dispersion slope estimated at this wavelength agree with the values reported by the manufacturer.
机译:在通过超短脉冲在光子晶体光纤中产生超连续谱的建模中,必须具有光纤的高阶色散项的知识,才能在模拟光谱和实验光谱之间取得良好的近似。但是,制造商通常不提供这些参数。在这项工作中,我们提出了带有六角孔的非线性光子晶体光纤的高阶色散项的数值估计。为了进行仿真,我们选择了具有高非线性响应的商用光纤(Blazephotonics NL-2.4-8)。光纤被设计为具有2.4μm的小纤芯直径,并且在包层中的空气孔呈三角形,间距为2.9μm。通过免费软件MIT Photonic Bands,可以对光纤的结构进行建模,并估算有效折射率以及色散项曲线。根据我们的结果,光纤的零色散波长为800游程,并且在该波长下,较高阶色散项为:β_2= 0,β_3= 0.05 ps〜3 / km,β_4= -7.03×l0 〜(-5)ps〜4 / km,β_5= 1.4×10〜(-7)ps5 / km,β_6= -4.163×10〜(-10)ps〜6 / km,β_7= 1.118×10〜(- 12)ps〜7 /公里。零色散波长和在该波长处估计的色散斜率与制造商报告的值一致。

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