0000000000484730

AUTHOR

Guillaume Canat

showing 11 related works from this author

Fourth order cascaded Raman shift in As38Se62 chalcogenide suspended core fiber pumped at 1.995 μm

2011

Fourth order cascaded Raman wavelength shift is demonstrated in As 38 Se 62 suspended core fiber using 1995 nm nanosecond source. The measured Raman gain coefficient is∼2×10−11 m/W at 1995 nm. The Raman peaks are reproduced by numerical simulations.

Materials sciencebusiness.industryChalcogenideNonlinear opticsNanosecondCore (optical fiber)chemistry.chemical_compoundsymbols.namesakeOpticschemistrysymbolsOptoelectronicsFiberbusinessRaman spectroscopyRefractive indexRaman scattering
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Recent developments in chalcogenide photonic crystal fibres

2011

Elaboration of low-losses highly non linear chalcogenide optical fibers for the generation of efficient non linear effects in the infrared remains a challenge. In recent years, much work has been devoted to the study of microstructured optical fibers (MOFs) with different designs and various elaboration processes. Their background losses were typically of several dB/m.

Optical fiberMaterials scienceInfraredbusiness.industryChalcogenidelaw.inventionPhotonic crystal fibreOptical pumpingPhase-change memorychemistry.chemical_compoundchemistrylawOptoelectronicsbusinessPhotonic-crystal fiberPhotonic crystal2011 IEEE Photonics Society Summer Topical Meeting Series
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Simulation of mid-IR amplification in Er3+-doped chalcogenide microstructured optical fiber

2009

International audience; This paper deals with the design of an erbium doped microstructured optical fiber (MOF) amplifier operating in the mid-infrared (mid-IR) wavelength range, more precisely around 4.5 µm wavelength. A homemade numerical code which solves the rate equations and the power propagation equations has been ad hoc developed to theoretically investigate the feasibility of mid-IR MOF amplifier. On the basis of the measured energy level transition parameters of a Er3+-doped Ga5Ge20Sb10S65 chalcogenide glass, the amplifier feasibility is demonstrated exhibiting high gain and low noise figure.

Finite element methodMaterials scienceOptical fiberChalcogenidePACS: 42.55.W 42.81.Q 42.60.D 02.70.Dchemistry.chemical_elementChalcogenide glassPhysics::Optics02 engineering and technology01 natural scienceslaw.invention010309 opticsInorganic ChemistryErbiumchemistry.chemical_compoundOpticslaw0103 physical sciencesElectrical and Electronic EngineeringPhysical and Theoretical ChemistryFinite element method; Photonic crystal fiber amplifiers; Rate equationsSpectroscopyAstrophysics::Galaxy Astrophysics[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryAmplifierOrganic ChemistryRate equationMicrostructured optical fiber021001 nanoscience & nanotechnologyPhotonic crystal fiber amplifiersAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsWavelengthRate equationschemistry0210 nano-technologybusiness
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Nonlinear effects above 2 µm in chalcogenide suspended core microstructured optical fibers: Modeling and experiments

2011

We present our latest results on the linear and nonlinear modeling, and on the fabrication of chalcogenide suspended core microstructured optical fibers for mid-infrared generation. We focus on an AsSe glass composition. We have used a thulium-doped fiber laser to pump our fibers around 2 µm. In order to enhance further the nonlinearities and to manage the chromatic dispersion for supercontinuum application, we have tapered some of our microstructured optical fibers.

PHOSFOSOptical fiberMaterials scienceChalcogenidebusiness.industryPhysics::OpticsMicrostructured optical fiberlaw.inventionSupercontinuumCondensed Matter::Materials Sciencechemistry.chemical_compoundOpticschemistrylawFiber laserDispersion (optics)businessPhotonic-crystal fiberIEEE Photonic Society 24th Annual Meeting
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Mid-infrared strong spectral broadening in microstructured tapered chalcogenide AsSe fiber

2012

We report on the generation of a supercontinuum in a chalcogenide microstructured tapered fiber. The suspended core diameter of the fiber is reduced from 5.5 μm to 0.8 μm in the waist of the tapered region. The zero dispersion wavelength is below 2 μm in the tapered region. To pump the fiber, we use a modelocked laser of 4 ps, with a central wavelength of 1960 nm. With only 150 W peak power in the fiber a supercontinuum is generated from 1300 to 2600 nm taking the supercontinuum wavelength edge at -30 dB from the continuum.

[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics]Materials scienceChalcogenide02 engineering and technology01 natural sciencesGraded-index fiber010309 opticschemistry.chemical_compoundOpticsZero-dispersion wavelengthFiber laser0103 physical sciencesDispersion-shifted fiberComputingMilieux_MISCELLANEOUS[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][CHIM.MATE] Chemical Sciences/Material chemistry[ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryMicrostructured optical fiber[CHIM.MATE]Chemical Sciences/Material chemistry021001 nanoscience & nanotechnologySupercontinuumchemistry[ CHIM.MATE ] Chemical Sciences/Material chemistry0210 nano-technologybusinessPhotonic-crystal fiber
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Low loss microstructured chalcogenide fibers for large non linear effects at 1995 nm

2010

International audience; Microstructured optical fibers (MOFs) are traditionally prepared using the stack and draw technique. In order to avoid the interfaces problems observed in chalcogenide glasses, we have developed a new casting method to prepare the chalcogenide preform. This method allows to reach optical losses around 0.4 dB/m at 1.55 µm and less than 0.05 dB/m in the mid IR. Various As(38)Se(62) chalcogenide microstructured fibers have been prepared in order to combine large non linear index of these glasses with the mode control offered by MOF structures. Small core fibers have been drawn to enhance the non linearities. In one of these, three Stokes order have been generated by Ram…

Materials scienceOptical fiberChalcogenide02 engineering and technology01 natural sciencesOCIS Codes : 060.2270 ; 060.2390 ; 060.4370 ; 160.2750 ; 060.4005law.invention010309 opticschemistry.chemical_compoundsymbols.namesakeOpticsStack (abstract data type)law0103 physical sciencesFiber Optic Technology[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryEquipment Design[CHIM.MATE]Chemical Sciences/Material chemistryMicrostructured optical fiber021001 nanoscience & nanotechnologyCastingAtomic and Molecular Physics and OpticsEquipment Failure AnalysisCore (optical fiber)Nonlinear Dynamicschemistry[ CHIM.MATE ] Chemical Sciences/Material chemistry[SPI.OPTI]Engineering Sciences [physics]/Optics / PhotonicsymbolsChalcogens[ SPI.OPTI ] Engineering Sciences [physics]/Optics / PhotonicGlass0210 nano-technologybusinessRaman scatteringPhotonic-crystal fiberOptics Express
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Fourth-order cascaded Raman shift in AsSe chalcogenide suspended-core fiber pumped at 2 μm

2011

International audience; Cascaded Raman wavelength shifting up to the fourth order ranging from 2092 to 2450nm is demonstrated using a nanosecond pump at 1995nm in a low-loss As38Se62 suspended-core microstructured fiber. These four Stokes shifts are obtained with a low peak power of 11W, and only 3W are required to obtain three shifts. The Raman gain coefficient for the fiber is estimated to (1.6 +-0.5)x 10e−11 m/W at 1995nm. The positions and the amplitudes of the Raman peaks are well reproduced by the numerical simulations of the nonlinear propagation.

Materials scienceOptical fibermoyen infrarougeChalcogenide02 engineering and technologyverre de chalcogénurecascades Raman01 natural scienceslaw.invention010309 opticssymbols.namesakechemistry.chemical_compoundOpticslawfibre optique microstucturée0103 physical sciencesFiber[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryoptique nonlinéaireNonlinear optics[CHIM.MATE]Chemical Sciences/Material chemistryNanosecond021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsCore (optical fiber)coeur suspenduchemistry[ CHIM.MATE ] Chemical Sciences/Material chemistrysymbols190.5650 060.4370 060.2390.0210 nano-technologyRaman spectroscopybusinessRaman scattering
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Er3+-doped GeGaSbS glasses for mid-IR fibre laser application: Synthesis and rare earth spectroscopy

2008

International audience; With an infrared transparency extended to 10 µm, low multiphonon relaxation rates and suitable rare earth solubility, sulphide glasses in the Ge-Ga-Sb-S system allow radiative emission from rare earth ions in the mid-IR range. The Er3+ ion, widely studied in glass fibres for optical amplification at 1.5 µm, presents an interesting transition for mid-IR applications around 4.5 µm (4I9/2→ 4I11/2). Thus, the aim of this work is to evaluate the Er3+-doped Ge20Ga5Sb10S65 glass as a potential fibre laser source operating in the 3-5 µm mid-IR spectral region. For that purpose, absorption and emission spectra were recorded from visible to mid-IR and the radiative lifetimes o…

Materials scienceChalcogenide glassesInfraredAnalytical chemistrychemistry.chemical_element02 engineering and technology01 natural sciences010309 opticsInorganic ChemistryErbiumOpticsOptical fibresFiber laser0103 physical sciencesRadiative transferEmission spectrumElectrical and Electronic EngineeringPhysical and Theoretical ChemistrySpectroscopyAbsorption (electromagnetic radiation)SpectroscopyMid-infrared[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryOrganic ChemistryFar-infrared laser021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materials42.70.Km; 42.55.Wd; 61.43.FschemistrySpectroscopic properties0210 nano-technologybusinessErbium
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Microstructured Optical Fibers from As2S3 Glass for Fiber Optics Sources in the MIR range

2011

International audience

[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics][PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][CHIM.MATE] Chemical Sciences/Material chemistry[ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics][ CHIM.MATE ] Chemical Sciences/Material chemistry[CHIM.MATE]Chemical Sciences/Material chemistryComputingMilieux_MISCELLANEOUS
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Nonlinear effects above 2 µm in chalcogenide suspended core microstructured optical fibers: modeling and experiments

2011

International audience

[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics][PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][CHIM.MATE] Chemical Sciences/Material chemistry[ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics][ CHIM.MATE ] Chemical Sciences/Material chemistry[CHIM.MATE]Chemical Sciences/Material chemistryComputingMilieux_MISCELLANEOUS
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Recent developments in chalcogenide PCF

2011

International audience

[PHYS.PHYS.PHYS-OPTICS] Physics [physics]/Physics [physics]/Optics [physics.optics][CHIM.MATE] Chemical Sciences/Material chemistry[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics][ CHIM.MATE ] Chemical Sciences/Material chemistry[CHIM.MATE]Chemical Sciences/Material chemistryComputingMilieux_MISCELLANEOUS
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