People | Locations | Statistics |
---|---|---|
Naji, M. |
| |
Motta, Antonella |
| |
Aletan, Dirar |
| |
Mohamed, Tarek |
| |
Ertürk, Emre |
| |
Taccardi, Nicola |
| |
Kononenko, Denys |
| |
Petrov, R. H. | Madrid |
|
Alshaaer, Mazen | Brussels |
|
Bih, L. |
| |
Casati, R. |
| |
Muller, Hermance |
| |
Kočí, Jan | Prague |
|
Šuljagić, Marija |
| |
Kalteremidou, Kalliopi-Artemi | Brussels |
|
Azam, Siraj |
| |
Ospanova, Alyiya |
| |
Blanpain, Bart |
| |
Ali, M. A. |
| |
Popa, V. |
| |
Rančić, M. |
| |
Ollier, Nadège |
| |
Azevedo, Nuno Monteiro |
| |
Landes, Michael |
| |
Rignanese, Gian-Marco |
|
Nilsson, Johan
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (26/26 displayed)
- 2024Amplification at 2.3-µm in 1.9-µm thulium-doped silica fiber laser
- 2021Binary acoustic trapping in a glass capillarycitations
- 2019An acoustofluidic platform for non-contact trapping of cell-laden hydrogel droplets compatible with optical microscopycitations
- 2018Validation of CryoSat-2 SARIn Data over Austfonna Ice Cap Using Airborne Laser Scanner Measurementscitations
- 2016Numerical methods for load and response prediction for use in acoustic fatigue
- 2014Numerical methods for load prediction in acoustic fatigue
- 2012Acoustic trapping with seed-particles for submicron particle enrichment.
- 2010100W CW cladding-pumped Raman fiber last at 1120nmcitations
- 2010Rare earth doped optical fiber fabrication using novel gas phase deposition techniquecitations
- 2010Bend-effects on Brillouin gain in large mode area fiber amplifiers with acoustic antiguide
- 2009Fiber design for high power fiber laserscitations
- 2009Ytterbium doped nanostructured optical fibers for high power fiber lasers
- 2008Reply to comment on “Photodarkening in Yb-doped aluminosilicate fibers induced by 488 nm irradiation”citations
- 2007Noninvasive acoustic cell trapping in a microfluidic perfusion system for online bioassayscitations
- 2007RGB generation by four-wave mixing in small-core holey fibers
- 2006Spectral control of optical gain in a rare earth-doped optical fiber using novel triple layered structurescitations
- 2006New Yb:Hf-doped silica fiber for high-power fiber laserscitations
- 2006Acoustic Trapping: System Design, Optimization and Applications
- 2006Temperature-dependent fluorescence characteristics of an ytterbium-sensitized erbium-doped silica fiber for sensor applicationscitations
- 2006Using Acoustic Differential Extraction to enhance analysis of sexual assualt evidence on a valveless glass microdevice
- 2004High-power wavelength-tunable cladding-pumped rare-earth-doped silica fiber laserscitations
- 2004Recent advances in high power fiber lasers
- 2004Passively Q-switched thulium-doped silica fiber laser
- 2004Thulium-ytterbium co-doped fiber laser with 32W of output power in the 2 micron wavelength range
- 2003Fiber lasers: flexible and functional solutions for today and the future
- 2002Synchronously pumped optical parametric oscillator driven by a femtosecond mode-locked fibre lasercitations
Places of action
Organizations | Location | People |
---|
conferencepaper
100W CW cladding-pumped Raman fiber last at 1120nm
Abstract
In recent years, rare-earth doped silica fiber lasers have become a popular medium to generate very high-power laser source, in particular in the 1 µm range where up to 10 kW single-mode ytterbium doped fiber (YDF) laser source has been reported and up to 0.9 kW from Tm doped fiber. The powers from other wavelengths are much lower typically between 10 to 100 W. An alternative to produce gain and power in optical fiber is to use nonlinear effect such as stimulated Raman scattering (SRS). SRS is wavelength agile, limited only by the transparency range of the fiber and the pump power wavelength. In addition, SRS sources benefit from low quantum defect, in particular at shorter wavelengths making them extremely efficient. However, because these effects rely on strong optical intensities to take place, fibers with small core size are typically used with core pumping scheme, limiting the scope for power scaling. Therefore, no very high power Raman fiber laser (RFL) has been reported and little progress has been made to increase the output power of those. As far as we are aware, the highest reported power from a core pumped RFL is about 68 W. There are several challenges in power scaling core-pumped Raman fiber laser, mainly the power handling capacity of single-mode fiber and the careful adjustment of the fiber length to avoid spurious 2nd order Stokes generation in the laser cavity.