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4.8微米充满一氧化碳的空芯石英光纤光源。

4.8-μm CO-filled hollow-core silica fiber light source.

作者信息

Li Xuanxi, Yang Linyong, Zhou Zhiyue, Li Zhixian, Li Hao, Pei Wenxi, Huang Wei, Shi Jing, Lei Luohao, Wang Meng, Wang Zefeng

机构信息

College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha, 410073, China.

Nanhu Laser Laboratory, National University of Defense Technology, Changsha, 410073, China.

出版信息

Light Sci Appl. 2024 Oct 18;13(1):295. doi: 10.1038/s41377-024-01615-x.

DOI:10.1038/s41377-024-01615-x
PMID:39420196
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC11487283/
Abstract

Mid-infrared (MIR) fiber lasers are important for a wide range of applications in sensing, spectroscopy, imaging, defense, and security. Some progress has been made in the research of MIR fiber lasers based on soft glass fibers, however, the emission range of rare-earth ions and the robustness of the host materials are still a major challenge for MIR fiber lasers. The large number of gases provide a variety of optical transitions in the MIR band. When combined with recent advances in low-loss hollow-core fiber (HCF), there is a great opportunity for gas-filled fiber lasers to further extend the radiation to the MIR region. Here, a 4.8-μm CO-filled silica-based HCF laser is reported for the first time. This is enabled by an in-house manufactured broadband low-loss HCF with a measured loss of 1.81 dB/m at 4.8 μm. A maximum MIR output power of 46 mW and a tuning range of 180 nm (from 4644 to 4824 nm) are obtained by using an advanced 2.33-μm narrow-linewidth fiber laser. This demonstration represents the longest-wavelength silica-based fiber laser to date, while the absorption loss of bulk silica at 4824 nm is up to 13, 000 dB/m. Further wavelength expansion could be achieved by changing the pump absorption line and optimizing the laser structure.

摘要

中红外(MIR)光纤激光器在传感、光谱学、成像、国防和安全等广泛应用中具有重要意义。基于软玻璃光纤的中红外光纤激光器的研究已经取得了一些进展,然而,稀土离子的发射范围和基质材料的稳健性仍然是中红外光纤激光器面临的主要挑战。大量气体在中红外波段提供了多种光学跃迁。当与低损耗空芯光纤(HCF)的最新进展相结合时,充气光纤激光器有很大机会将辐射进一步扩展到中红外区域。在此,首次报道了一种4.8μm的充CO二氧化硅基空芯光纤激光器。这是通过内部制造的宽带低损耗空芯光纤实现的,该光纤在4.8μm处测得的损耗为1.81dB/m。通过使用先进的2.33μm窄线宽光纤激光器,获得了46mW的最大中红外输出功率和180nm(从4644到4824nm)的调谐范围。这一演示代表了迄今为止波长最长的二氧化硅基光纤激光器,而块状二氧化硅在4824nm处的吸收损耗高达13000dB/m。通过改变泵浦吸收线和优化激光器结构,可以实现进一步的波长扩展。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/d4e621898767/41377_2024_1615_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/416b9684fb50/41377_2024_1615_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/2c2ec637bbda/41377_2024_1615_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/359a3712f120/41377_2024_1615_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/24973effe1c0/41377_2024_1615_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/f9cdc8d354f0/41377_2024_1615_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/d4e621898767/41377_2024_1615_Fig6_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/416b9684fb50/41377_2024_1615_Fig1_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/2c2ec637bbda/41377_2024_1615_Fig2_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/359a3712f120/41377_2024_1615_Fig3_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/24973effe1c0/41377_2024_1615_Fig4_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/f9cdc8d354f0/41377_2024_1615_Fig5_HTML.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/2e88/11487283/d4e621898767/41377_2024_1615_Fig6_HTML.jpg

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本文引用的文献

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4.3 µm high-power amplified spontaneous emission fiber source based on CO-filled nested hollow-core anti-resonant fiber.基于充CO的嵌套空心反谐振光纤的4.3微米高功率放大自发辐射光纤源。
Opt Express. 2024 Apr 8;32(8):14532-14540. doi: 10.1364/OE.517713.
2
2.3-µm single-frequency Tm: ZBLAN fiber amplifier with output power of 1.41 W.输出功率为1.41瓦的2.3微米单频掺铥氟锆酸盐光纤放大器。
Opt Express. 2023 Nov 20;31(24):40991-40999. doi: 10.1364/OE.508003.
3
3.1 W mid-infrared fiber laser at 4.16 µm based on HBr-filled hollow-core silica fibers.
基于填充 HBr 的中空芯石英光纤的 3.1μm 中红外光纤激光器。
Opt Lett. 2022 Nov 15;47(22):5785-5788. doi: 10.1364/OL.475690.
4
High-gain single-frequency Tm-doped ZBLAN fiber amplifier at 2.33 μm.2.33μm 高增益单频 Tm 掺杂 ZBLAN 光纤放大器。
Opt Lett. 2023 Jan 15;48(2):502-505. doi: 10.1364/OL.480084.
5
Prospects and applications of on-chip lasers.片上激光器的前景与应用
eLight. 2023;3(1):1. doi: 10.1186/s43593-022-00027-x. Epub 2023 Jan 4.
6
Fiber laser source of 8 W at 3.1 µm based on acetylene-filled hollow-core silica fibers.基于充乙炔空芯石英光纤的3.1微米波长8瓦光纤激光源。
Opt Lett. 2022 May 1;47(9):2354-2357. doi: 10.1364/OL.457265.
7
Gas fiber lasers may represent a breakthrough in creating powerful radiation sources in the mid-IR.气体光纤激光器可能代表着在中红外波段创建强大辐射源方面的一项突破。
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15 W monolithic fiber laser at 3.55 µm.波长为3.55微米的15瓦单块光纤激光器。
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Light Sci Appl. 2022 Jan 13;11(1):15. doi: 10.1038/s41377-021-00703-6.
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Appl Opt. 2021 Sep 20;60(27):8550-8555. doi: 10.1364/AO.435274.