Search results for "43"

showing 10 items of 1438 documents

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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Optical and Vibrational Spectra of CsCl-Enriched GeS2-Ga2S3 Glasses

2016

Optical and FTIR spectroscopy was employed to study the properties of 80GeS2-20Ga2S3-CsCl chalcohalide glasses with CsCl additives in a temperature range of 77–293 K. It is shown that CsCl content results in the shift of fundamental absorption edge in the visible region. Vibrational bands in FTIR spectra of (80GeS2-20Ga2S3)100 − х (СsCl) x (x = 5, 10, and 15) are identified near 2500 cm−1, 3700 cm−1,, around 1580 cm−1, and a feature at 1100 cm−1. Low energy shifts of vibrational frequencies in glasses with a higher amount of CsCl can be caused by possible thermal expansion of the lattice and nanovoid agglomeration formed by CsCl additives in the inner structure of the Ge-Ga-S glass.

Materials scienceChalcohalide glassChalcogenideAnalytical chemistryNanochemistry02 engineering and technologyModification01 natural sciencesThermal expansionVibrational propertieschemistry.chemical_compound78.70.BjMaterials Science(all)Lattice (order)0103 physical sciencesGeneral Materials ScienceFourier transform infrared spectroscopy010302 applied physicsNano ExpressChalcogenide61.43.Fs71.23.CqAtmospheric temperature rangeOptical spectra021001 nanoscience & nanotechnologyCondensed Matter Physics81.70PgchemistryAbsorption edge82.56Ub0210 nano-technologyVibrational spectraNanoscale Research Letters
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On-surface synthesis on a bulk insulator surface

2018

On-surface synthesis has rapidly emerged as a most promising approach to prepare functional molecular structures directly on a support surface. Compared to solution synthesis, performing chemical reactions on a surface offers several exciting new options: due to the absence of a solvent, reactions can be envisioned that are otherwise not feasible due to the insolubility of the reaction product. Perhaps even more important, the confinement to a two-dimensional surface might enable reaction pathways that are not accessible otherwise. Consequently, on-surface synthesis has attracted great attention in the last decade, with an impressive number of classical reactions transferred to a surface as…

Materials scienceInsulator (electricity)02 engineering and technology010402 general chemistryF160 Organic Chemistry53001 natural sciencesChemical reactionUllmann reactionMetalchemistry.chemical_compoundGeneral Materials ScienceF200 Materials ScienceDiacetylene021001 nanoscience & nanotechnologyCondensed Matter PhysicsCycloaddition0104 chemical sciencesPolymerizationchemistryChemical physicsvisual_artvisual_art.visual_art_mediumF343 Computational PhysicsF320 Chemical PhysicsSupport surface0210 nano-technologyJournal of Physics: Condensed Matter
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Laser beam scattering effects in non-absorbent inhomogenous polymers

2007

Ilie, Mariana Kneip, Jean-Christophe Mattei, Simone Nichici, Alexandru Roze, Claude Girasole, Thierry; In this paper a numerical model for laser beam scattering in the semi-transparent polymers is presented, using a Monte Carlo algorithm and the Mie theory. The algorithm correctly accounts for the independent multiply-scattered light. We describe the algorithm, present a number of important parameters that account in the welding process, and explicitly show how the algorithm can be used to estimate the laser beam intensity both inside the semi-transparent component and at the welding interface and the beam widening. For the model validation an experimental bench test has been realized and s…

Materials scienceMonte Carlo method02 engineering and technologyWelding01 natural sciencesBeam parameter productlaw.invention010309 opticsOpticslaw0103 physical sciencesElectrical and Electronic EngineeringMonte Carlo algorithmbusiness.industryMechanical EngineeringLaser beam welding021001 nanoscience & nanotechnologyAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic Materials[SPI.OPTI]Engineering Sciences [physics]/Optics / PhotonicPhysics::Accelerator PhysicsM squaredLaser beam quality0210 nano-technologybusiness0143-8166Beam (structure)
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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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Theory of parabolic pulse propagation in nonlinear dispersion decreasing optical fiber amplifiers

2008

Optical fibers ; Nonlinear optics ; Optical fiber amplifiers ; Optical amplifier ; Optical solitons ; Electromagnetic wave propagation ; Pulse propagation ;; International audience; We show that pulse spectral broadening in normally dispersive nonlinear fiber amplifiers may be enhanced by introducing a suitable dispersion tapering. We obtain an analytical dispersion profile that permits one to reduce pulse propagation in a varying dispersion fiber to the case of an equivalent fiber with constant parameters.

Materials sciencePhysics::OpticsDispersion (waves); fibers; nonlinear opticsPolarization-maintaining optical fiber02 engineering and technologyfibers01 natural sciencesGraded-index fiber010309 optics020210 optoelectronics & photonicsDouble-clad fiberOptics190.4370 190.55300103 physical sciencesDispersion (optics)0202 electrical engineering electronic engineering information engineeringDispersion-shifted fiberDispersion (waves)Self-phase modulation[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics][ PHYS.PHYS.PHYS-OPTICS ] Physics [physics]/Physics [physics]/Optics [physics.optics]business.industrynonlinear opticsSingle-mode optical fiberStatistical and Nonlinear PhysicsAtomic and Molecular Physics and OpticsbusinessBandwidth-limited pulse
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Vibrations of free and embedded anisotropic elastic spheres:Application to low-frequency Raman scattering of silicon nanoparticles in silica

2004

Vibrational mode frequencies and damping are calculated for an elastic sphere embedded in an infinite, homogeneous, isotropic elastic medium. Anisotropic elasticity of the sphere significantly shifts the frequencies in comparison to simplified calculations that assume isotropy. New low-frequency Raman light scattering data are presented for silicon spheres grown in a ${\mathrm{SiO}}_{2}$ glass matrix. Principal features of the Raman spectrum are not correctly described by a simple model of the nanoparticle as a free, isotropic sphere, but require both matrix effects and the anisotropy of the silicon to be taken into account. Libration, not vibration, is the dominant mechanism.

Materials scienceSilicon[ PHYS.COND.CM-MS ] Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]FOS: Physical scienceschemistry.chemical_element02 engineering and technology01 natural sciencesMolecular physicsLight scatteringsymbols.namesakeOptics0103 physical sciencesLibration010306 general physicsAnisotropy63.22.+m78.30.-j43.20.+g02.70.NsCondensed Matter - Materials Sciencebusiness.industryIsotropyMaterials Science (cond-mat.mtrl-sci)021001 nanoscience & nanotechnologyCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsX-ray Raman scatteringchemistrysymbols[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]0210 nano-technologyRaman spectroscopybusinessRaman scattering
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Parabolic pulse generation with active or passive dispersion decreasing optical fibers

2007

International audience; We experimentally demonstrate the possibility to generate parabolic pulses via a single dispersion decreasing optical fiber with normal dispersion. We numerically and experimentally investigate the influence of the dispersion profile, and we show that a hybrid configuration combining dispersion decrease and gain has several benefits on the parabolic generated pulses.

Materials sciencebusiness.industry02 engineering and technology01 natural sciencesGraded-index fiberAtomic and Molecular Physics and Optics010309 optics020210 optoelectronics & photonicsOpticsZero-dispersion wavelengthPolarization mode dispersiondispersion (waves); light pulse generators; optical gain0103 physical sciencesDispersion (optics)0202 electrical engineering electronic engineering information engineeringModal dispersionDispersion-shifted fiberbusiness060.4370 060.5530 320.5540Ultrashort pulseBandwidth-limited pulse
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PANI-Based Wearable Electrochemical Sensor for pH Sweat Monitoring

2021

Nowadays, we are assisting in the exceptional growth in research relating to the development of wearable devices for sweat analysis. Sweat is a biofluid that contains useful health information and allows a non-invasive, continuous and comfortable collection. For this reason, it is an excellent biofluid for the detection of different analytes. In this work, electrochemical sensors based on polyaniline thin films deposited on the flexible substrate polyethylene terephthalate coated with indium tin oxide were studied. Polyaniline thin films were abstained by the potentiostatic deposition technique, applying a potential of +2 V vs. SCE for 90 s. To improve the sensor performance, the electronic…

Materials scienceelectrochemical sensor02 engineering and technologySubstrate (electronics)QD415-436wearable sensor010402 general chemistry01 natural sciencespH meterBiochemistryreduced graphene oxidepolyanilineAnalytical ChemistryContact anglechemistry.chemical_compoundPolyanilineSettore ING-IND/17 - Impianti Industriali MeccanicipH sensorPhysical and Theoretical ChemistryThin filmSettore ING-IND/34 - Bioingegneria Industriale021001 nanoscience & nanotechnology0104 chemical sciencesElectrochemical gas sensorIndium tin oxidesweatSettore ING-IND/23 - Chimica Fisica ApplicataChemical engineeringchemistryElectrode0210 nano-technologyChemosensors
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