纳秒脉冲混合铥-拉曼光纤放大器2.1 $\mu\ mathm {m}$

André W. Edvardsen, L. G. Holmen
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引用次数: 0

摘要

工作在2.1 μm左右的激光源在遥感、自由空间光通信、国防和医学等领域具有广泛的应用前景。最常见的是,使用掺铥光纤激光器在1.95 μm处泵浦掺钬光纤来达到该光谱范围,但一些研究表明,掺钬光纤放大器的效率远低于理论上可能的效率[1]。凑巧的是,2.1μm波长接近1.95μm泵浦的拉曼位移峰值(~ 13 THz)。这意味着可以开发出2.1 μm光(称为Stokes)可以通过无源光纤中的受激拉曼散射(SRS)而不是通过掺ho光纤中的受激发射来放大的放大器。
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Nanosecond-Pulsed Hybrid Thulium-Raman Fiber Amplifier at 2.1 $\mu\mathrm{m}$
Laser sources operating around 2.1 μm are attractive for a range of applications in areas such as remote sensing, free-space optical communication, defense and medicine. Most commonly, holmium-doped fibers pumped by thulium-doped fiber lasers at 1.95 μm are used to reach this spectral regime, but several studies have shown that holmium-doped fiber amplifiers have a much lower efficiency than theoretically possible [1]. Coincidentally, the wavelength 2.1μm lies close to the peak Raman shift (~ 13 THz in silica) of the 1.95μm pump. This means that amplifiers can be developed where 2.1 μm light (called Stokes) could be amplified through stimulated Raman scattering (SRS) in a passive fiber instead of through stimulated emission in a Ho-doped fiber.
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