Ultraviolet to mid-infrared gas-filled anti-resonant hollow-core fiber lasers

被引:0
作者
Wang, Yazhou [1 ]
Adamu, Abubakar, I [1 ]
Habib, Md Selim [2 ,3 ]
Dasa, Manoj K. [1 ]
Petersen, Christian R. [1 ,5 ]
Antonio-Lopez, J. Enrique
Zhou, Binbin [1 ]
Jepsen, Peter Uhd [1 ,5 ]
Schulzgen, Axel [2 ]
Bache, Morten [1 ]
Correa, Rodrigo Amezcua [2 ]
Bang, Ole [1 ,4 ,5 ]
Markos, Christos [1 ,5 ]
机构
[1] Tech Univ Denmark, DTU Foton, DK-2800 Lyngby, Denmark
[2] Univ Cent Florida, Coll Opt & Photon, CREOL, Orlando, FL 32816 USA
[3] Florida Polytech Univ, Dept Elect & Comp Engn, Lakeland, FL 33805 USA
[4] NKT Photon, Blokken 84, DK-3460 Birkerod, Denmark
[5] NORBLIS IVS, Virumgade 35D, DK-2830 Virum, Denmark
来源
MICRO-STRUCTURED AND SPECIALTY OPTICAL FIBRES VII | 2021年 / 11773卷
关键词
Anti-resonant hollow-core fiber; supercontinuum; Raman laser; STIMULATED RAMAN-SCATTERING; PHOTONIC CRYSTAL FIBERS; MU-M; PEAK POWER; MID-IR; DEPENDENCE; GENERATION; DEUTERIUM; HYDROGEN; PULSES;
D O I
10.1117/12.2592717
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
We will present our recent works on fiber lasers enabled by noble and Raman-active gas-filled anti-resonant hollow-core fiber (ARHCF) technology. First, we will present the generation of supercontinuum (SC) spanning from 200 nm to 4 mu m based on a Argon (Ar)-filled ARHCF pumped at 2.46 mu m wavelength with 100 fs pulses and similar to 8 mu J pulse energy. Then we will discuss our recent work on stimulated Raman scattering (SRS) effect in a hydrogen (H-2)-filled ARHCF, to achieve infrared Raman lasers. By employing the single-stage vibrational SRS effect, a 4.22 mu m Raman laser line is directly converted from a linearly polarized 1.53 mu m pump laser. A quantum efficiency as high as 74% was achieved, to yield 17.6 mu J pulse energy. The designed 4.22 mu m wavelength is overlapped with the strongest CO2 absorption, therefore constituting a promising way for CO2 detection. In addition, we report a multi-wavelength Raman laser based on cascaded rotational SRS effect. Four Raman lines at 1683 nm, 1868 nm, 2099 nm, and 2394 nm are generated, with pulse energies as high as 18.25 mu J, 14.4 mu J, 14.1 mu J, and 8.2 mu J, respectively. The energy of these Raman lines can be controlled by tuning the H-2 pressure from 1 bar to 20 bar.
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页数:7
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