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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Ebendorff-Heidepriem, Heike
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Topics
Publications (11/11 displayed)
- 2023Controlled formation of gold nanoparticles with tunable plasmonic properties in tellurite glasscitations
- 2022Impact of rare earth doping on the luminescence of lanthanum aluminum silicate glasses for radiation sensing
- 2021Extruded suspended core fibers from lanthanum-aluminum-silicate glass
- 2019Micron scale thermometry using lanthanide doped tellurite glass
- 2019Effects of pressurization and surface tension on drawing Ge-Sb-Se chalcogenide glass suspended-core fibercitations
- 2018Stack-and-draw microstructured optical fiber with Ge28Sb12Se60 chalcogenide glasscitations
- 2017Extrusion of fluid cylinders of arbitrary shape with surface tension and gravitycitations
- 2016Microstructured Optical Fiber-based Biosensorscitations
- 2011Midinfrared optical rogue waves in soft glass photonic crystal fibercitations
- 2011Energy level decay and excited state absorption processes in erbium-doped tellurite glasscitations
- 2006Non-silica microstructured optical fibers for mid-IR supercontinuum generation from 2 µm - 5 µmcitations
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document
Non-silica microstructured optical fibers for mid-IR supercontinuum generation from 2 µm - 5 µm
Abstract
We have performed numerical simulations to investigate the optimization of compound glass microstructured optical fibers for mid IR supercontinuum generation beyond the low loss transmission window of silica, using pump wavelengths in the range 1.55-2.25 µm. <br/>Large mode area fibers for high powers, and small core fiber designs for low powers, are proposed for a variety of glasses. Modeling results showed that for Bismuth and lead oxide glasses, which have nonlinearities ~10 x that of silica, matching the dispersion profile to the pump wavelength is essential. For chalcogenide glasses, which have much higher nonlinearities, the dispersion profile is less important. <br/>The pump pulses have duration of <1 ps, and energy <30 nJ. The fiber lengths required for generating continuum were <40 mm, so the losses of the fibers were not a limiting factor. Compared to planar rib-waveguides or fiber-tapers, microstructured fiber technology has the advantages of greater flexibility for tailoring the dispersion profile over a broad wavelength span, and a much wider possible range of device lengths.