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具有宽带发光的铒/镱共掺杂氟碲酸盐玻璃光纤

Er/Yb Co-Doped Fluorotellurite Glass Fiber with Broadband Luminescence.

作者信息

Zhu Hepan, Xu Weisheng, Fan Zhichao, Bai Shengchuang, Zhang Peiqing, Dai Shixun, Nie Qiuhua, Shen Xiang, Wang Rongping, Wang Xunsi

机构信息

Laboratory of Infrared Materials and Devices, Advanced Technology Research Institute, Ningbo University, Ningbo 315211, China.

Zhejiang Key Laboratory of Photoelectric Materials and Devices, Ningbo 315211, China.

出版信息

Sensors (Basel). 2024 Aug 14;24(16):5259. doi: 10.3390/s24165259.

DOI:10.3390/s24165259
PMID:39204953
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11359483/
Abstract

In order to address the 'capacity crisis' caused by the narrow bandwidth of the current C band and the demand for wide-spectrum sensing sources and tunable fiber lasers, a broadband luminescence covering the C + L bands using Er/Yb co-doped fluorotellurite glass fiber is investigated in this paper. The optimal doping concentrations in the glass host were determined based on the intensity, lifetime, and full width at half maximum (FWHM) of the fluorescence centered at 1.5 µm, which were found to be 1.5 mol% ErO and 3 mol% YbO. We also systematically investigated this in terms of optical absorption spectra, absorption and emission cross-sections, gain coefficients, Judd-Ofelt parameters, and up-conversion fluorescence. The energy transfer (ET) mechanism between the high concentrations of Er and Yb was summarized. In addition, a step-indexed fiber was prepared based on these fluorotellurite glasses, and a wide bandwidth of ~112.5 nm (covering the C + L bands from 1505.1 to 1617.6 nm) at 3 dB for the amplified spontaneous emission (ASE) spectra has been observed at a fiber length of 0.57 m, which is the widest bandwidth among all the reports based on tellurite glass. Therefore, this kind of Er/Yb co-doped fluorotellurite glass fiber has great potential for developing broadband C + L band amplifiers, ultra-wide fiber sources for sensing, and tunable fiber lasers.

摘要

为了解决当前C波段带宽狭窄以及对广谱传感源和可调谐光纤激光器的需求所导致的“容量危机”,本文研究了一种采用铒/镱共掺杂氟碲酸盐玻璃光纤覆盖C+L波段的宽带发光。基于以1.5μm为中心的荧光强度、寿命和半高宽(FWHM)确定了玻璃基质中的最佳掺杂浓度,发现分别为1.5mol%的ErO和3mol%的YbO。我们还从光吸收光谱、吸收和发射截面、增益系数、Judd-Ofelt参数以及上转换荧光等方面对其进行了系统研究。总结了高浓度铒和镱之间的能量转移(ET)机制。此外,基于这些氟碲酸盐玻璃制备了一种阶跃折射率光纤,在0.57m的光纤长度下,观察到放大自发辐射(ASE)光谱在3dB时具有约112.5nm的宽带宽(覆盖从1505.1到1617.6nm的C+L波段),这是基于碲酸盐玻璃的所有报道中最宽的带宽。因此,这种铒/镱共掺杂氟碲酸盐玻璃光纤在开发宽带C+L波段放大器、超宽传感光纤源和可调谐光纤激光器方面具有巨大潜力。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/fd218ff120f7/sensors-24-05259-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/0fb34af5bfa3/sensors-24-05259-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/cb23b9dd71e2/sensors-24-05259-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/903a8fba1f99/sensors-24-05259-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/88e58da0f8b7/sensors-24-05259-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/53c5573ec149/sensors-24-05259-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/114379cedfa9/sensors-24-05259-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/fd218ff120f7/sensors-24-05259-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/0fb34af5bfa3/sensors-24-05259-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/cb23b9dd71e2/sensors-24-05259-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/903a8fba1f99/sensors-24-05259-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/88e58da0f8b7/sensors-24-05259-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/53c5573ec149/sensors-24-05259-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/114379cedfa9/sensors-24-05259-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/e173/11359483/fd218ff120f7/sensors-24-05259-g007.jpg

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本文引用的文献

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Opt Express. 2023 Aug 28;31(18):28850-28858. doi: 10.1364/OE.496574.
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