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首页> 外文期刊>Laser Physics: An International Journal devoted to Theoretical and Experimental Laser Research and Application >All-normal-dispersion dissipative-soliton fiber laser at 1.06 μm using a bulk-structured Bi_2Te_3 topological insulator-deposited side-polished fiber
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All-normal-dispersion dissipative-soliton fiber laser at 1.06 μm using a bulk-structured Bi_2Te_3 topological insulator-deposited side-polished fiber

机译:使用体结构化Bi_2Te_3拓扑绝缘子沉积侧抛光光纤的1.06μm全正色散耗散孤子光纤激光器

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摘要

We experimentally demonstrate a 1.06-μm dissipative-soliton fiber laser incorporating a saturable absorber based on a bulk-structured Bi_2Te_3 topological insulator (TI). The saturable absorber, which had a bulk-structured Bi_2Te_3 TI film deposited on a side-polished fiber, provided the dual functions of nonlinear saturable absorption and spectral comb filtering, which are essential for the generation of dissipative solitons. The saturable absorption function was obtained through a micrometer-thick bulk-structured Bi_2Te_3 TI film, whereas the spectral comb filtering function was through the asymmetric side-polished fiber structure, on top of which a different refractive index film was deposited. The ~17 μm-thick Bi_2Te_3 TI film was prepared using a simple mechanical exfoliation method. The fabrication of the targeted micrometer-thick bulk-structured film was straightforward without needing special care, compared to nanosheet-based film fabrication. Stable dissipative-soliton pulses with a composite temporal shape were readily obtained by incorporating the prepared saturable absorber into an ytterbium-doped fiber ring cavity with all-normal dispersion. The temporal width of the output pulses was measured to be ~230 ps.
机译:我们通过实验证明了一个1.06-μm的耗散孤子光纤激光器,该激光器结合了基于体结构Bi_2Te_3拓扑绝缘体(TI)的可饱和吸收体。具有饱和结构的Bi_2Te_3 TI薄膜沉积在侧面抛光的光纤上的可饱和吸收剂提供了非线性可饱和吸收和光谱梳状滤波的双重功能,这对于产生耗散孤子至关重要。可饱和吸收功能是通过微米厚的块状Bi_2Te_3 TI薄膜获得的,而光谱梳状滤波功能是通过不对称的侧面抛光纤维结构获得的,在该纤维上沉积了不同的折射率薄膜。使用简单的机械剥落方法制备〜17μm厚的Bi_2Te_3 TI膜。与基于纳米片的薄膜制造相比,目标微米级厚的整体结构薄膜的制造简单明了,无需特别注意。通过将制备的可饱和吸收剂掺入具有全法向色散的掺ped光纤环腔中,可以容易地获得具有复合时间形状的稳定的耗散孤子脉冲。测量输出脉冲的时间宽度为〜230 ps。

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