Fluoride Fibers
Supercontinuum generation fibers
Thanks two their non linear properties, combined to their high transparency from UV up to mid-IR, fluoride fibers are widely used for supercontinuum generation:
In 2006 the first supercontinuum generation, extending from 0.8 up to 4.5µm was demonstrated from LVF ZBLAN fluoride fibers by Xia et al. [ref].
ZFG and IFG fluoride fibers are integrated in the commercial supercontinuum source Electro-MIR 4100 and Electro-MIR 4800, developed in colaboration with LEUKOS.
Our two star fibers for supercontinuum generation are:
1) ZFG SM [2.55] 8.5/125
Core/clad diameter
Cutoff wavelength
Numerical aperture
Zero Dispersion Wavelength
Non linear refractive index n2 (x 10-20 m²/W)
Operating wavelength
Typical background loss
8.5/125 µm
2.55 µm
0.23
1.535 µm (experimental)
≈ 2.1
0.3 – 4.5 µm
< 10 dB/km
Consult our fluoride fibers/general proprerties section to learn more about this fiber.
Find below the wavelength dependence of core and cladding refractive indices of our 8.5/125 non linear fiber:
Here are some supercontinuum results obtained with our ZFG singlemode fibers thanks to their non linearity:
Spectral broadening | Average power | Ref |
|---|---|---|
0.8 – 4.5 µm | 0.023 W | Xia, 2006 |
0.8 – 4.0 µm | 1.3 W | Xia, 2007 |
2.6 – 4.1 µm | 0.154 W | Gauthier 2015 |
2 – 4.70 µm | – | Michalska 2017 |
2 – 4.4 µm | 2.45 W | Grzes 2018 |
2.7 – 4.25 µm | 1.75 W | Yang, 2018 |
1.9 – 4.0 µm | 5.4 W | Xia, 2020 |
1.92 – 4.29 µm | 20.6 W | Yang, 2020 |
2) IFG SM [2.95] 7.5/125
Core/clad diameter
Cutoff wavelength
Numerical aperture
Zero Dispersion Wavelength
Non linear refractive index n2 (x 10-20 m²/W)
Operating wavelength
Typical background loss
7.5/125 µm
2.95 µm
0.30
1.65 µm (experimental)
≈ 3.2-4.3 [ref]
0.3 – 5.5 µm
< 35 dB/km
Consult our fluoride fibers/general proprerties section to learn more about this fiber.
Find below the wavelength dependence of core and cladding refractive indices of our 7.5/125 non linear fiber:
Here are some supercontinuum results obtained with our IFG singlemode fibers thanks to their non linearity:
Spectral broadening | Average power | Ref |
|---|---|---|
2.7 – 4.7 µm | – | Théberge, 2013 |
1.0 – 3.05 µm | 2.09 W | Swiderski, 2014 |
2.4 – 5.4 µm | 0.008 W | Gauthier, 2016 |
1 – 5 µm | 1.0 W | Théberge, 2018 |
2.6 – 5.4 µm | 0.145 W | Gauthier 2018 |
1.85 – 4.1 µm | 1.41 W | Michalska 2018 |
1.5 – 5.2 µm | 1.35 W | Yang 2018 |
1.9 – 5.1 µm | 4.06 W | |
1.8 – 4.6 µm | 3.0 W | Yehouessi, 2019 |
– | 6.7 W | |
2 – 4.7 µm | 7.0 W | Scurria, 2020 |
1.9 – 4.9 µm | 11.8 W | Yang, 2020 |
We acknowledge LEUKOS for ZDW measurements.
We acknowledge Glass and Ceramics team from Rennes 1 University for their contribution to refractive index measurements
