Search results for " Scattering"

showing 10 items of 6840 documents

Phosphorous doping and drawing effects on the Raman spectroscopic properties of O=P bond in silica-based fiber and preform.

2012

International audience; We report an experimental study of the doping and drawing effects on the Raman activities of phosphorus (P)-doped silica-based optical fiber and its related preform. Our data reveal a high sensitivity level in the full width at half maximum value of the 1330 cm−1 (O = P) Raman band to the P-doping level. Its increase with the P doping level does not clash with an increase in the disorder of the O = P surrendering matrix. In addition, we observe that in the central core region of the sample (higher doping level), the drawing process decreases the relative band amplitude. We tentatively suggest that this phenomenon is due to the change in the first derivate of the bond…

(060.2310) Fiber optics; (300.6450) Spectroscopy Raman; (160.2750) Glass and other amorphous materials; (060.2280) Fiber design and fabrication; (060.2290) Fiber materials.inorganic chemicalsMaterials scienceOptical fiberAnalytical chemistryChemical vapor depositionlaw.inventionCondensed Matter::Materials Sciencesymbols.namesakeOpticslawPolarizabilityCondensed Matter::SuperconductivityFiber[PHYS.PHYS.PHYS-OPTICS]Physics [physics]/Physics [physics]/Optics [physics.optics]business.industryDopingtechnology industry and agricultureFiber optics Spectroscopy Raman Glass and other amorphous materials Fiber design and fabrication Fiber materialsElectronic Optical and Magnetic MaterialsFull width at half maximumsymbolsbusinessRaman spectroscopyhuman activitiesRaman scattering
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"Table 1" of "The e+ e- ---> pi+ pi- pi+ pi-, K+ K- pi+ pi-, and K+ K- K+ K- cross sections at center-of-mass energies 0.5-GeV to 4.5-GeV measured…

2006

Measured PI+ PI- PI+ PI- cross sections. The errors are statistical only.

0.613-4.45E+ E- --> PI+ PI- PI+ PI-E+ E- ScatteringIntegrated Cross SectionExclusiveCross SectionSIG
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Molecular association of cryptand 221D in NaCl-water solutions. A small-angle neutron scattering study

1993

Molecules of 5-Decyl-4,7,13,16,21-pentaoxa-1,10-diaza-bicyclo-[8.8.5.]tricosan (221D) and its sodium complex, with both a hydrophobic and a hydrophilic portion, are expected to form aggregates in water solutions. This was confirmed by surface tension measurements. The aggregation behaviour was studied by small-angle neutron scattering at two different [NaCl]/[221D] molar ratios, such as to obtain, in one case, aggregates entirely made up of ionic monomers, and in the other, mixed micelles constituted by both ionic and non-ionic units. The variation of the aggregation number and number of aggregates indicated that, in the former case, smaller micelles were formed, as a consequence of repulsi…

010302 applied physicsAggregation numberAqueous solutionChemistryCryptandGeneral Physics and AstronomyIonic bonding02 engineering and technologyNeutron scattering021001 nanoscience & nanotechnology01 natural sciencesMicelleSmall-angle neutron scatteringSurface tensionCrystallography[PHYS.HIST]Physics [physics]/Physics archives0103 physical sciences0210 nano-technologyLe Journal de Physique IV
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Irradiation effects in CaF2probed by Raman scattering

2016

The formation conditions and dynamics of Ca colloids and point defects that appear in irradiated single crystals of CaF2 were investigated by Raman spectroscopy. The intensity changes in the Raman spectra because of the presence of different concentrations of point defects and Ca colloids that emerged in CaF2 after irradiation with 2.2 GeV Au ions were used to study their distribution and stability under illumination with three laser wavelengths (473, 532 and 633 nm) at different output powers (2 to 200 mW). A damage saturation at a fluence of 6 × 1011 ion cm−2 was observed. The dependence of the spectral changes on the ion fluence can be described by a core/halo damage cross-section model.…

010302 applied physicsChemistryAnalytical chemistry02 engineering and technology021001 nanoscience & nanotechnologyLaser01 natural sciencesCrystallographic defectMolecular physicsFluencelaw.inventionIonsymbols.namesakeSwift heavy ionlaw0103 physical sciencessymbolsGeneral Materials ScienceIrradiation0210 nano-technologyRaman spectroscopySpectroscopyRaman scatteringJournal of Raman Spectroscopy
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Bandgap behavior and singularity of the domain-induced light scattering through the pressure-induced ferroelectric transition in relaxor ferroelectri…

2018

[EN] In this letter, we have investigated the electronic structure of A(x)Ba(1-x)Nb(2)O(6) relaxor ferroelectrics on the basis of optical absorption spectroscopy in unpoled single crystals with A = Sr and Ca under high pressure. The direct character of the fundamental transition could be established by fitting Urbach's rule to the photon energy dependence of the absorption edge yielding bandgaps of 3.44(1) eV and 3.57(1) eV for A = Sr and Ca, respectively. The light scattering by ferroelectric domains in the pre-edge spectral range has been studied as a function of composition and pressure. After confirming with x-ray diffraction the occurrence of the previously observed ferroelectric to pa…

010302 applied physicsDiffractionPhase transitionMaterials sciencePhysics and Astronomy (miscellaneous)Absorption spectroscopyCondensed matter physics02 engineering and technologyPhoton energy021001 nanoscience & nanotechnology01 natural sciencesFerroelectricityLight scatteringCRYSTALSTEMPERATURE-DEPENDENCEAbsorption edgeCALCIUM BARIUM NIOBATEFISICA APLICADA0103 physical sciencesDirect and indirect band gaps0210 nano-technologyCALCIUM BARIUM NIOBATE TEMPERATURE-DEPENDENCE CRYSTALS
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Nonlinear optical response of bulk ZnO crystals with different content of intrinsic defects

2018

Abstract The nonlinear optical (NLO) properties of native defect-rich ZnO single crystals were studied in details within the excitation of the continuous wave (CW) and pulsed laser radiation at 532 nm (2.33 eV). Analysis of the experimental data of optical elastic scattering, Fourier transform infrared (FTIR), near infrared–visible–ultraviolet (NIR–Vis–UV) spectra recorded in reflection and absorption modes, and data of photoluminescence (PL) spectroscopy confirmed the contribution of both intrinsic defects and their clusters, being determined before by neutron diffraction and XRD analysis. It was shown that the high sensitivity of the NLO diagnostics via self-action of a laser beam is due …

010302 applied physicsElastic scatteringMaterials sciencePhotoluminescenceInfraredOrganic ChemistryNeutron diffraction02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesMolecular physicsAtomic and Molecular Physics and OpticsLight scatteringElectronic Optical and Magnetic MaterialsInorganic ChemistryWavelength0103 physical sciencesElectrical and Electronic EngineeringPhysical and Theoretical ChemistryFourier transform infrared spectroscopy0210 nano-technologySpectroscopySpectroscopyOptical Materials
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RBS and ERD cross-sections and optical model parameters for the analysis of lithium, boron and nickel

2000

Abstract Elastic scattering cross-sections for RBS analysis of nickel by 7 Li and 11 B ion backscattering near the Coulomb barrier have been determined. The lithium ion measurements were performed in the energy range of 8–15 MeV at the laboratory angles of 115° and 135°. For boron ions the energies between 14 and 24 MeV and scattering angles of 89°, 110° and 130° were used. For the analysis of lithium and boron by ERD the scattering cross-sections have been calculated by kinematically reversing the backscattering process. The calculated 58 Ni ion energies thus varied between 65 and 125 MeV for lithium and between 75 and 130 MeV for boron recoils. For the Li + Ni and B + Ni systems the thres…

010302 applied physicsElastic scatteringNuclear and High Energy PhysicsScatteringchemistry.chemical_elementCoulomb barrier02 engineering and technology021001 nanoscience & nanotechnology7. Clean energy01 natural sciencesIonNickelsymbols.namesakechemistry0103 physical sciencessymbolsLithiumRutherford scatteringAtomic physics0210 nano-technologyBoronInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Neutron scattering and imaging: a tool for archaeological studies

2015

International audience; Neutron scattering and neutron imaging are powerful techniques for studying the structure of objects without damage, which is an essential prerequisite for investigations in Cultural Heritage domain, particularly in Archaeology. The deep penetration of neutrons in most materials allows for the study of relatively large objects. The contrast between similar materials, like metals in alloys, or that due to the presence of hydrogen atoms gives information about the internal structure of objects that have been modified or repaired in the past. Imaging and tomography give a 3-dimensional view of the whole object, permitting discrimination between different parts of the ob…

010302 applied physicsElemental compositionMaterials sciencebusiness.industryNeutron imagingneutron scatteringDeep penetrationQuantitative EvaluationsStructure02 engineering and technologyNeutron scattering021001 nanoscience & nanotechnology01 natural sciencesArchaeology[SPI]Engineering Sciences [physics]OpticsArchaeologyGeochemistry and PetrologyNeutron imaging0103 physical sciencesNeutronPorous materialsTomography0210 nano-technologybusiness
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Raman characterization of Pb2Na1−xLaxNb5−xFexO15 and Pb0.5(5−x)LaxNb5−xFexO15 (0≤x≤1) solid solutions

2011

Abstract The ferroelectric compounds Pb 2 Na 1− x La x Nb 5− x Fe x O 15 and Pb 0.5(5− x ) La x Nb 5− x Fe x O 15 (0≤ x ≤1) with the tungsten bronze type structure have been investigated using Raman spectroscopy. The evolution of the spectra as a function of composition at room temperature is reported. In the frequency range 200–1000 cm −1 three main A 1 phonons around 240 ( υ 1 ), 630 ( υ 2 ) and 816 ( υ 3 ) cm −1 were observed. The broadening of the Raman lines for high values of x originates from a significant structural disorder. This is in good agreement with the relaxor character of these compositions. The lowest-frequency part of the spectra, below 180 cm −1 , reveals a structural ch…

010302 applied physicsMaterials science[ PHYS.COND.CM-MS ] Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]Analytical chemistrychemistry.chemical_element02 engineering and technologyAtmospheric temperature rangeTungsten021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencesFerroelectricitySpectral lineElectronic Optical and Magnetic Materialssymbols.namesakechemistry0103 physical sciences[PHYS.COND.CM-MS]Physics [physics]/Condensed Matter [cond-mat]/Materials Science [cond-mat.mtrl-sci]symbolsElectrical and Electronic Engineering0210 nano-technologySpectroscopyRaman spectroscopyRaman scatteringSolid solutionPhysica B: Condensed Matter
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Lattice sites of diffused gold and platinum in epitaxial ZnSe layers

2000

Abstract The lattice location of diffused gold and platinum in zinc selenide (ZnSe) epitaxial layers was studied using the Rutherford backscattering (RBS) channeling technique. Thin Au and Pt films were evaporated onto ZnSe samples. The Au/ZnSe samples were annealed at 525°C and the residual Au film was removed by etching. Channeling angular scan measurements showed that about 30% of Au atoms were close to substitutional site (displaced about 0.2 A). In the case of the Pt/ZnSe samples the annealing temperatures ranged from 600°C to 800°C. The Pt minimum yields along 〈1 0 0〉 direction were close to the random value, varying from 80% to 90%. The measured Pt angular scans along 〈1 0 0〉 and 〈1 …

010302 applied physicsNuclear and High Energy PhysicsMaterials scienceScatteringAnnealing (metallurgy)chemistry.chemical_element02 engineering and technologyAtmospheric temperature range021001 nanoscience & nanotechnologyEpitaxy01 natural sciencessymbols.namesakechemistry.chemical_compoundCrystallographyTransition metalchemistry0103 physical sciencessymbolsZinc selenideRutherford scattering0210 nano-technologyPlatinumInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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