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Tailoring bandgap transmission spectra of new Neodymium-doped tellurite all-solid photonic bandgap fibers with double cladding layers

机译:新型掺钕碲酸盐全固态双包层光子带隙光纤的定制带隙透射谱

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摘要

Neodymium (Nd)-doped fibers are potential candidates for optical fiber amplifiers operating near the 1.3-μm spectralregion due to the ~4F_(3/2)→~4I_(13/2) transition of Nd~(3+) ions. But, there is an amplified spontaneous emission at 1.06 μm due tothe ~4F_(3/2)→~4I_(11/2) transition whose branching ratio is about 5 times larger than that at 1.3 μm. In order to suppress thetransmission of the 1.06-μm emission, we propose a new tellurite all-solid photonic bandgap fiber (ASPBF) with a singleline of high index rods and double cladding layers. Tellurite glasses of TeO_2-Li_2O-WO_3-MoO_3-Nb_2O_5 (TLWMN), TeO_2-ZnO-Na_2O-La_2O_3 (TZNL) and TeO_2-ZnO-Li_2O-K_2O-Al_2O_3-P_2O_5 (TZLKAP) are developed. High-index rods ofTLWMN and an Nd-doped TZNL rod are arranged symmetrically and horizontally in the x-axis of a hexagonal TZNLcladding. The outer cladding is made of the TZLKAP glass. The finite element method is used to calculate the modedistribution and the bandgap properties. The fiber transmission spectra are numerically investigated with the effects ofrod diameter and filling factor variation. When the core diameter is 3.0 μm, rod diameter is 2.3 μm and filling factor isfrom 0.7 to 0.8, the 1.06-μm emission which is caused by the ~4F_(3/2)→~4I_(11/2) transition can be suppressed as compared withthe 1.33-μm emission which is caused by the ~4F_(3/2)→~4I_(13/2) transition.
机译:由于Nd〜(3+)的〜4F_(3/2)→〜4I_(13/2)跃迁,掺钕(Nd)的光纤是在1.3μm光谱\ r \ n区域工作的光纤放大器的潜在候选者。 )离子。但是,由于〜4F_(3/2)→〜4I_(11/2)跃迁,在1.06μm处存在放大的自发发射,其分支比约为1.3μm处的5倍。为了抑制1.06-μm发射的传输,我们提出了一种新的亚碲酸盐全固态光子带隙光纤(ASPBF),它具有单根高折射率棒和双层包层。开发了TeO_2-Li_2O-WO_3-MoO_3-Nb_2O_5(TLWMN),TeO_2- \ r \ nZnO-Na_2O-La_2O_3(TZNL)和TeO_2-ZnO-Li_2O-K_2O-Al_2O_3-3-P_2O_5(TZLKAP)的碲酸盐玻璃。 \ r \ nTLWMN高折射率棒和Nd掺杂的TZNL棒在六角形TZNL \ r \ n包层的x轴上对称且水平地排列。外包层由TZLKAP玻璃制成。有限元方法用于计算模式\ r \ n分布和带隙属性。对纤维传输光谱进行了数值研究,并考察了杆直径和填充系数的变化。当芯径为3.0μm,棒径为2.3μm,填充系数为\ r \ n从0.7至0.8时,由〜4F_(3/2)→〜4I_(11/2)引起的1.06-μm发射与〜4F_(3/2)→〜4I_(13/2)过渡引起的1.33-μm发射相比,可以抑制过渡。

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  • 来源
    《Optical Components and Materials XVI》|2019年|109141O.1-109141O.6|共6页
  • 会议地点 0277-786X;1996-756X
  • 作者单位

    Research Center for Advanced Photon Technology, Toyota Technological Institute, 2-12-1 Hisakata, Tempaku-ku, Nagoya, 468-8511, Japan tonghoangtuan@gmail.com;

    Research Center for Advanced Photon Technology, Toyota Technological Institute, 2-12-1 Hisakata, Tempaku-ku, Nagoya, 468-8511, Japan;

    Research Center for Advanced Photon Technology, Toyota Technological Institute, 2-12-1 Hisakata, Tempaku-ku, Nagoya, 468-8511, Japan;

    Research Center for Advanced Photon Technology, Toyota Technological Institute, 2-12-1 Hisakata, Tempaku-ku, Nagoya, 468-8511, Japan;

    Research Center for Advanced Photon Technology, Toyota Technological Institute, 2-12-1 Hisakata, Tempaku-ku, Nagoya, 468-8511, Japan;

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