Search results for "backscatter"

showing 10 items of 123 documents

Ion irradiation of AZO thin films for flexible electronics

2017

Aluminum doped Zinc oxide (AZO) is a promising transparent conductor for solar cells, displays and touch-screen technologies. The resistivity of AZO is typically improved by thermal annealing at temperatures not suitable for plastic substrates. Here we present a non-thermal route to improve the electrical and structural properties of AZO by irradiating the TCO films with O+ or Ar+ ion beams (30–350 keV, 3 × 1015–3 × 1016 ions/cm2) after the deposition on glass and flexible polyethylene naphthalate (PEN). X-ray diffraction, optical absorption, electrical measurements, Rutherford Backscattering Spectrometry and Atomic Force Microscopy evidenced an increase of the crystalline grain size and a …

Nuclear and High Energy PhysicsMaterials science02 engineering and technology01 natural sciencesSettore ING-INF/01 - ElettronicaSettore FIS/03 - Fisica Della MateriaOpticsTransparent conductive oxideElectrical resistivity and conductivity0103 physical sciencesAZO ; Transparent conductive oxide ; Ion implantationElectrical measurementsThin filmPolyethylene naphthalateFlexible and transparent electronicInstrumentationTransparent conducting filmNuclear and High Energy Physic010302 applied physicsbusiness.industryAZO021001 nanoscience & nanotechnologyRutherford backscattering spectrometryIon implantationIon implantationOptoelectronicsCrystallite0210 nano-technologybusinessPhotovoltaic
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Formation of cobalt silicide from filter metal vacuum arc deposited films

2006

The thermal reaction of Co film deposited on Si(111) surfaces by a high current filter metal vacuum arc (FMEVAD) system has been studied. After deposition the films were annealed over the 400-900 degrees C temperature range for 30 min. Rutherford backscattering spectrometry (RBS) was used to characterize the elemental depth distributions in the films subjected to different annealing temperatures. Ordered chemical phases were determined by glancing-incidence X-ray diffraction (GIXRD) and the morphology was determined by cross section transmission electron microscopy (TEM). The results show that the phases formed are Co2Si at 400 degrees C, CoSi + Coo at 500 degrees C, CoSi + CoSi2 at 600 deg…

Nuclear and High Energy PhysicsMaterials scienceAnnealing (metallurgy)Analytical chemistrychemistry.chemical_elementVacuum arcRutherford backscattering spectrometryAmorphous solidCrystallographychemistry.chemical_compoundchemistryTransmission electron microscopySilicideInstrumentationCobaltCobalt oxideNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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A study of solar thermal absorber stack based on CrAlSiNx/CrAlSiNxOy structure by ion beams

2019

Renewable energies are foreseen as a major energy resource for next generations. Among several energy sources and technologies available, Concentrated Solar Power (CSP) technology has a great potential, but it needs to be optimised, in particular to reduce the costs, with an increase of the operating temperature and long term stability. This goal can be achieved by tailoring the composition and multilayer structure of films. In this work we present and discuss the results obtained from solar absorber coatings based on nitride/oxynitride structures. A four-layer film structure, W/CrAlSiNx(HA)/CrAlSiNxOy(LA)/SiAlOx, was deposited on stainless steel substrates using magnetron sputtering deposi…

Nuclear and High Energy PhysicsMaterials scienceCrAlSiNx /CrAlSiNxOy02 engineering and technologyaurinkoenergia010402 general chemistry01 natural sciences7. Clean energyRutherford Backscattering Spectrometry (RBS)time of flight elastic recoil detection analysis (TOF-ERDA)Operating temperatureSputteringConcentrated solar power:Engenharia dos Materiais [Engenharia e Tecnologia]Thermal stabilityCrAlSiN /CrAlSiN O x x yInstrumentationpinnoitteetTime of flight Elastic Recoil Detection Analysis (TOF-ERDA)CrAlSiNx/CrAlSiNxOyScience & TechnologySolar selective absorberbusiness.industrySputteringSolar selective absorber ; Rutherford Backscattering Spectrometry (RBS) ; Time of flight Elastic Recoil Detection Analysis (TOF-ERDA) ; CrAlSiNx/CrAlSiNxOySputteringSputter deposition021001 nanoscience & nanotechnologyRutherford backscattering spectrometry0104 chemical sciencesElastic recoil detectionsolar selective absorberspektrometriaEngenharia e Tecnologia::Engenharia dos MateriaisOptoelectronicssputteringohutkalvot0210 nano-technologybusinessEnergy source
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Ordering effects in extreme high-resolution depth profiling with MeV ion beams

2012

Abstract The continuing development of depth profiling with MeV ion beam methods with depth resolutions in the nanometre, and even sub-nanometre, regime implies the resolved depth become comparable with the interatomic spacing. To investigate how short-range ordering influences depth profiles at these resolutions, we have employed a mathematical modelling approach. The radial, g ( r ) and depth distribution, g ( z ) functions were calculated for (1 0 0) surface, random and amorphous Si structures at 300 K produced using molecular dynamics simulations with the EDIP quasi-empirical potential. The results showed that short-range ordering lead to reduction of the scattering yield below the deep…

Nuclear and High Energy PhysicsMaterials scienceIon beamta114business.industryScatteringRutherford backscattering spectrometryRadial distribution functionMolecular physicsIonElastic recoil detectionMolecular dynamicsOpticsbusinessInstrumentationAtomic spacingNuclear Instruments and Methods in Physics Research B
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Characterization of alpha sources prepared by direct evaporation using Rutherford backscattering spectrometry

1997

Abstract Standardization of solutions containing alpha emitting nuclides by direct evaporation onto metal supports is a widely used technique due to its simplicity in providing good quantitative results. In order to avoid inhomogeneity in the deposition surface, polished stainless steel disks and a spreading agent are generally used. These sources are usually measured by alpha spectrometry using passivated implanted silicon detectors. The resolution of the source is a measure of the thickness and homogeneity of the evaporated layer. Rutherford backscattering of He+ and H+ was here used to measure directly this thickness and homogeneity. The results were in agreement with semiconductor detec…

Nuclear and High Energy PhysicsMaterials scienceSiliconAlpha spectrometryPhysics::Instrumentation and DetectorsDetectorAnalytical chemistrychemistry.chemical_elementRutherford backscattering spectrometrySemiconductor detectorMetalchemistryvisual_artHomogeneity (physics)visual_art.visual_art_mediumNuclideInstrumentation
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Synthesis and characterization of cobalt silicide films on silicon

2006

Cobalt silicide has emerged as a leading contact material in silicon technology due to its low resistivity, high stability and small lattice mismatch. In this study, 0.2-0.4 mu m thick Co films were deposited on Si(100) wafers by RF magnetron sputtering at room temperature, and annealed at temperatures from 600 to 900 degrees C in vacuum. As-deposited and annealed samples were characterized by Rutherford backscattering spectrometry (RBS), nuclear reaction analysis (NRA), X-ray diffraction (XRD) and scanning electron microscopy (SEM). Although the Si substrates were sputter cleaned before the deposition, all the samples showed a thin oxide layer at the Si/Co interfaces. Annealing up to 700 d…

Nuclear and High Energy PhysicsMaterials scienceSiliconScanning electron microscopeAnnealing (metallurgy)Analytical chemistrychemistry.chemical_elementSputter depositionRutherford backscattering spectrometrychemistrySputteringElectrical resistivity and conductivityNuclear reaction analysisInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Characterization of 233U alpha recoil sources for 229()Th beam production

2019

Radioactive $^{233}$U alpha recoil sources are being considered for the production of a thorium ion source to study the low-energy isomer in $^{229}$Th with high-resolution collinear laser spectroscopy at the IGISOL facility of the University of Jyv\"askyl\"a. In this work two different $^{233}$U sources have been characterized via alpha and gamma spectroscopy of the decay radiation obtained directly from the sources and from alpha-recoils embedded in implantation foils. These measurements revealed rather low $^{229}$Th recoil efficiencies of only a few percent. Although the low efficiency of one of the two sources can be attributed to its inherent thickness, the low recoil efficiency of th…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsMaterials sciencePhysics::Instrumentation and Detectors010308 nuclear & particles physicsRadioactive sourceFOS: Physical sciencesThoriumchemistry.chemical_elementInstrumentation and Detectors (physics.ins-det)RadiationRutherford backscattering spectrometry01 natural sciencesIon sourceRecoilchemistry0103 physical sciencesGamma spectroscopyNuclear Experiment (nucl-ex)Atomic physicsNuclear Experiment010306 general physicsSpectroscopyNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The MATHUSLA test stand

2020

The rate of muons from LHC $pp$ collisions reaching the surface above the ATLAS interaction point is measured and compared with expected rates from decays of $W$ and $Z$ bosons and $b$- and $c$-quark jets. In addition, data collected during periods without beams circulating in the LHC provide a measurement of the background from cosmic ray inelastic backscattering that is compared to simulation predictions. Data were recorded during 2018 in a 2.5 $\times$ 2.5 $\times$ 6.5~$\rm{m}^3$ active volume MATHUSLA test stand detector unit consisting of two scintillator planes, one at the top and one at the bottom, which defined the trigger, and six layers of RPCs between them, grouped into three $(x…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsBackscattered cosmic raysLong-lived particles; LHC; MATHUSLA; Backscattered cosmic raysFOS: Physical sciencesCosmic rayScintillator01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)0103 physical sciencesmedicineDetectors and Experimental Techniques010306 general physicsphysics.ins-detInstrumentationSettore FIS/01PhysicsLuminosity (scattering theory)MuonLarge Hadron ColliderInteraction pointhep-ex010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)Long-lived particlesMATHUSLAmedicine.anatomical_structureW′ and Z′ bosonsHigh Energy Physics::ExperimentLHCParticle Physics - ExperimentNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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On the metal distribution in the system GeTe−Sb2Te3

1988

The structures of GeSb2Te4, Ge2Sb2Te5 and GeSb4Te7 are not determined completely by means of classical X-ray or electron diffraction studies. We have measured the Mossbauer parameters of121Sb in these compounds as well as in their binary constituent Sb2Te3 as an attempt to improve our knowledge on the question.

Nuclear and High Energy PhysicsReflection high-energy electron diffractionMössbauer effectChemistryAnalytical chemistryCrystal structureCondensed Matter PhysicsAtomic and Molecular Physics and OpticsMetalCrystallographyDistribution (mathematics)Electron diffractionvisual_artMössbauer spectroscopyvisual_art.visual_art_mediumPhysical and Theoretical ChemistryElectron backscatter diffractionHyperfine Interactions
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Time-of-flight telescope for heavy-ion RBS

2007

Abstract This paper describes a time-of-flight (TOF) spectrometer for Heavy-Ion Rutherford Backscattering Spectrometry (HI-RBS) recently installed at IMEC for thin film analysis. The TOF telescope allows the use of ion beams heavier than He, with advantages in terms of depth and mass resolution and sensitivity compared to conventional RBS based on planar Si detectors. The start timing-signal is produced by the secondary electrons emitted from a thin C foil when traversed by a backscattered ion; the electrons are deflected in an electrostatic mirror towards a Micro-channel plate (MCP) assembly which provides a fast timing response. The stop signal is obtained directly from a second MCP assem…

Nuclear and High Energy PhysicsSpectrometerPhysics::Instrumentation and Detectorsbusiness.industryChemistryRutherford backscattering spectrometrySecondary electronslaw.inventionIonElastic recoil detectionTelescopeTime of flightOpticslawTime-of-flight mass spectrometrybusinessInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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