Third-order cascaded Raman shift in all-solid fluorotellurite fiber pumped at 1550 nm

In this Letter, we demonstrate a third-order cascaded Raman shift in an all-solid fluorotellurite fiber pumped by a 1550 nm nanosecond laser. The fluorotellurite glass with a composition of TeO -BaF -Y O (TBY) has a usable Raman shift of ∼785 cm and a Raman gain coefficient of ∼1.65 × 10 m/W at 1550...

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Veröffentlicht in:Optics letters 2022-02, Vol.47 (3), p.690-693
Hauptverfasser: Jiao, Yadong, Jia, Zhixu, Guo, Xiaohui, Zhao, Zhipeng, Ohishi, Yasutake, Qin, Weiping, Qin, Guanshi
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Sprache:eng
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Zusammenfassung:In this Letter, we demonstrate a third-order cascaded Raman shift in an all-solid fluorotellurite fiber pumped by a 1550 nm nanosecond laser. The fluorotellurite glass with a composition of TeO -BaF -Y O (TBY) has a usable Raman shift of ∼785 cm and a Raman gain coefficient of ∼1.65 × 10 m/W at 1550 nm, which is approximately 25.4 times larger than that of silica glass. By using a 5.38 m fluorotellurite fiber as the Raman gain medium and a 1550 nm nanosecond laser as the pump light, a third-order cascaded Raman shift is obtained via spontaneous cascaded Raman amplification in the fluorotellurite fiber, causing the generation of the first-, second-, and third-order Stokes emissions that peak at 1765, 2049, and 2438 nm, respectively. For an average pump power of ∼491.5 mW, the output power of the generated first-, second-, and third-order Stokes light is approximately 14.1, 67.4, and 31.6 mW, respectively. The corresponding conversion efficiency is approximately 2.87%, 13.70%, and 6.43%, respectively. Our results show that fluorotellurite fibers are promising Raman gain media for constructing cascaded Raman fiber lasers with a wide range of wavelengths.
ISSN:0146-9592
1539-4794
DOI:10.1364/OL.446730