Search results for "width [Lambda(1405)]"

showing 10 items of 330 documents

In-situ monitoring by Raman spectroscopy of the thermal doping of graphene and MoS2 in O-2-controlled atmosphere

2017

The effects of temperature and atmosphere (air and O2) on the doping of monolayers of graphene (Gr) on SiO2 and Si substrates, and on the doping of MoS2 multilayer flakes transferred on the same substrates have been investigated. The investigations were carried out by in situ micro-Raman spectroscopy during thermal treatments up to 430 °C, and by atomic force microscopy (AFM). The spectral positions of the G and 2D Raman bands of Gr undergo only minor changes during treatment, while their amplitude and full width at half maximum (FWHM) vary as a function of the temperature and the used atmosphere. The thermal treatments in oxygen atmosphere show, in addition to a thermal effect, an effect a…

Controlled atmosphereMaterials science2Analytical chemistrythermal dopingGeneral Physics and Astronomychemistry.chemical_elementtwo-dimensional (2D) materials02 engineering and technologyMoSlcsh:Chemical technology010402 general chemistrylcsh:Technology01 natural sciencesOxygenFull Research Paperlaw.inventionPhysics and Astronomy (all)symbols.namesakelawMonolayerNanotechnologylcsh:TP1-1185General Materials ScienceElectrical and Electronic Engineeringlcsh:ScienceSpectroscopylcsh:TGrapheneSettore FIS/01 - Fisica SperimentaleDopinggraphenetechnology industry and agriculture021001 nanoscience & nanotechnologylcsh:QC1-9990104 chemical sciencesNanoscienceFull width at half maximumTwo-dimensional (2D) materialchemistryRaman spectroscopysymbolslcsh:QMaterials Science (all)0210 nano-technologyRaman spectroscopyMoS2lcsh:Physics
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Zero Ripple Current with Coupled Inductors in Continuous Conduction Mode under PWM Signals

2020

This article presents a generalized analysis to explain current ripple of an $m$ windings coupled inductor with a given coupling factor $k_{ij}$ for each pair of windings and then studies more in detail its use in the continuous conduction mode and with pulsewidth modulated signals. To determine the current ripple, a generalized expression of the equivalent inductance of each winding is calculated, including the influence of voltage unbalance. In the ideal case, the equivalent inductance shows that the current ripple can only become $m$ times smaller than that with uncoupled inductors. But in the unbalanced case, some divergences of the equivalent inductance appear that are responsible for …

CouplingPhysicsEnginyeria elèctrica020208 electrical & electronic engineeringEquivalent series inductanceRippleEnergy Engineering and Power Technology02 engineering and technologyInductorTopologyInductanceElectromagnetic coil0202 electrical engineering electronic engineering information engineeringElectrical and Electronic EngineeringPulse-width modulationVoltage
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Radiation damage in zircon

2003

A single, zoned, Sri Lankan zircon exhibits a range of microstructures from crystalline to nearly amorphous that are the result of radiation damage over a dose range of 2.1–10.1·1015 α-decay events/mg (0.16–0.47 dpa). The zones in the crystal were examined at a variety of length scales using optical microscopy, micro-Raman spectroscopy, electron microprobe analysis, and transmission electron microscopy. Birefringence varies linearly with dose: birefringence = −4.71·10−18 /g· D α + 4.86·10−2. Full width at half maximum (FWHM) measurements of the B1g(ν3) peak, as determined by micro-Raman spectroscopy, were used to estimate the extent of radiation damage in each zone. The radiation dose (calc…

CrystalFull width at half maximumGeophysicsGeochemistry and PetrologyTransmission electron microscopyAnalytical chemistryRadiation damageMineralogyElectron microprobeSpectroscopyGeologyZirconAmorphous solidAmerican Mineralogist
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Photoluminescence excited by ArF and KrF lasers and optical absorption of stishovite mono-crystal

2008

Two photoluminescence bands were found in a stishovite (silicon dioxide) mono-crystal sample under ArF (193 nm) and KrF (248 nm) excitation. The blue band is situated at 3.17 ± 0.02 eV in the case of ArF and at 3 ± 0.2 in the case of KrF. The UV band is at 4.55 ± 0.05 eV in the case of ArF and at 4.5 ± 0.05 eV in the case of KrF. The position of the UV emission band correlates with that excited by x rays. This position is 4.6 ± 0.05 eV with FWHM 0.8 ± 0.05 eV (Truhins et al 2003 Solid State Commun. 127 415). The blue band possesses slow decay kinetics with time constant 16 ± 2 µs and the UV band is fast on the level of 2 ± 0.5 ns, similarly for both lasers. Thermal quenching of both bands b…

CrystalFull width at half maximumPhotoluminescenceChemistryExcited stateGeneral Materials ScienceIrradiationAtomic physicsCondensed Matter PhysicsLuminescenceAbsorption (electromagnetic radiation)StishoviteJournal of Physics: Condensed Matter
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Experimental realization of a pillared metasurface for flexural wave focusing

2021

International audience; A metasurface is an array of subwavelength units with modulated wave responses that show great potential for the control of refractive/reflective properties in compact functional devices. In this work, we propose an elastic metasurface consisting of a line of pillars with gradient heights, erected on a homogeneous plate. The change in the resonant frequencies associated with the height gradient allows us to achieve transmitted phase response covering a range of 2π, while the amplitude response remains at a relatively high level. We employ the pillared units to design a focusing metasurface and compare the properties of the focal spots through simulation and experimen…

DiffractionMaterials scienceFabricationQC1-999Physics::Optics02 engineering and technologyInterference (wave propagation)01 natural sciences[SPI.MAT]Engineering Sciences [physics]/MaterialsOpticsRobustness (computer science)0103 physical sciencesPhase responseFocal lengthGeneral Materials Science[SPI.NANO]Engineering Sciences [physics]/Micro and nanotechnologies/Microelectronics010302 applied physics[SPI.ACOU]Engineering Sciences [physics]/Acoustics [physics.class-ph]business.industryPhysicsGeneral Engineering021001 nanoscience & nanotechnologyTransverse planeFull width at half maximum0210 nano-technologybusinessTP248.13-248.65Biotechnology
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High-energy X-ray diffraction and topography investigation of CdZnTe

2005

High-energy transmission x-ray diffraction techniques have been applied to investigate the crystal quality of CdZnTe (CZT). CdZnTe has shown excellent performance in hard x-ray and gamma detection; unfortunately, bulk nonuniformities still limit spectroscopic properties of CZT detectors. Collimated high-energy x-rays, produced by a superconducting wiggler at the National Synchrotron Light Source’s X17B1 beamline, allow for a nondestructive characterization of thick CZT samples (2–3 mm). In order to have complete information about the defect distribution and strains in the crystals, two series of experiments have been performed. First, a monochromatic 67 keV x-ray beam with the size of 300×3…

DiffractionMaterials sciencebusiness.industryWigglerSynchrotron radiationCondensed Matter PhysicsCollimated lightElectronic Optical and Magnetic MaterialsCrystalFull width at half maximumOpticsradiation detectorsBeamlineCadmium alloysMaterials ChemistryCadmium tellurideElectrical and Electronic EngineeringRaster scanbusinessJournal of Electronic Materials
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Enhanced supercontinuum generation in tapered tellurite suspended core fiber

2015

Abstract We demonstrate 400-THz (0.6–3.3 µm) bandwidth infrared supercontinuum generation in a 10 cm-long tapered tellurite suspended core fiber pumped by nJ-level 200-fs pulses from an optical parametric oscillator. The increased nonlinearity and dispersion engineering extended by the moderate reduction of the fiber core size are exploited for supercontinuum optimization on both frequency edges (i.e., 155-THz overall gain), while keeping efficient power coupling into the untapered fiber input. The remaining limitation of supercontinuum bandwidth is related to the presence of the high absorption beyond 3 µm whereas spectral broadening is expected to fully cover the glass transmission window…

Dispersion engineeringMaterials scienceInfraredbusiness.industryBandwidth (signal processing)Nonlinear opticsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsSupercontinuumOpticsOptical parametric oscillatorElectrical and Electronic EngineeringPhysical and Theoretical ChemistrybusinessHigh absorptionDoppler broadeningOptics Communications
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Near-intrinsic energy resolution for 30-662 keV gamma rays in a high pressure xenon electroluminescent TPC

2013

We present the design, data and results from the NEXT prototype for Double Beta and Dark Matter (NEXT-DBDM) detector, a high-pressure gaseous natural xenon electroluminescent time projection chamber (TPC) that was built at the Lawrence Berkeley National Laboratory. It is a prototype of the planned NEXT-100 Xe-136 neutrino-less double beta decay (0 nu beta beta) experiment with the main objectives of demonstrating near-intrinsic energy resolution at energies up to 662 keV and of optimizing the NEXT-100 detector design and operating parameters. Energy resolutions of similar to 1% FWHM for 662 keV gamma rays were obtained at 10 and 15 atm and similar to 5% FWHM for 30 keV fluorescence xenon X-…

ElectroluminiscènciaNuclear and High Energy PhysicsXenonHigh-pressureDark matterchemistry.chemical_elementNuclear physicsTECNOLOGIA ELECTRONICAXenonDouble beta decayEnergy resolutionNeutrinoless double beta decayInstrumentationPhysicsTime projection chamberDetectorResolution (electron density)Gamma rayFísicaNuclear energyFull width at half maximumchemistryElectroluminescenceEnergia nuclearTPC
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Stark broadening of the hydrogen Paschen ? transition at electron densities of the order of $ \mathsf {10^{15}}$ cm $ \mathsf {^{-3}}$

2003

Stark broadening measurements and calculations of the Paschen γ spectral line of hydrogen ( λ = 1.094[: MU :] m) are reported. Investigations have been performed at plasma electron densities between 1.4×10 15 cm -3 and 3.7×10 15 cm -3 . As the light source a wall-stabilized arc operated in a helium-hydrogen gas mixture at atmospheric pressure has been applied. The radiation of the plasma emitted from nearly homogeneous plasma layers in end-on direction, was measured with the use of a grating spectrometer equipped with a charge coupled device (CCD) detector. The radiance calibration was carried out against light outputs originating from a tungsten strip radiation standard. The measured FWHM …

Electron densityFull width at half maximumsymbols.namesakeMaterials scienceAtmospheric pressureStark effectsymbolsPlasma diagnosticsElectronPlasmaAtomic physicsAtomic and Molecular Physics and OpticsSpectral lineThe European Physical Journal D - Atomic, Molecular and Optical Physics
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Calibration of the width of the NI spectral line at for electron density determination

2002

Abstract The Stark broadening of a NI spectral line at 7915.42 A has been calibrated for electron density determination of low temperature plasmas. The determined simple formula based on measured FWHM is applicable in the electron density range from 3×1015 to 10 16 cm −3 .

Electron densityRange (particle radiation)RadiationMaterials sciencePlasmaAtomic and Molecular Physics and OpticsSpectral lineFull width at half maximumsymbols.namesakeStark effectCalibrationsymbolsAtomic physicsSpectroscopyJournal of Quantitative Spectroscopy and Radiative Transfer
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