Search results for "scattering [p nucleus]"

showing 10 items of 198 documents

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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Chiral unitary approach to eta'N scattering at low energies

2010

We study the \eta' N interaction within a chiral unitary approach which includes \pi N, \eta N and related pseudoscalar meson-baryon coupled channels. Since the SU(3) singlet does not contribute to the standard interaction and the \eta' is mostly a singlet, the resulting scattering amplitude is very small and inconsistent with experimental estimations of the \eta' N scattering length. The additional consideration of vector meson-baryon states into the coupled channel scheme, via normal and anomalous couplings of pseudoscalar to vector mesons, enhances substantially the \eta' N amplitude. We also exploit the freedom of adding to the Lagrangian a new term, allowed by the symmetries of QCD, wh…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryHigh Energy Physics::LatticeNuclear Theory01 natural sciencesQuantum mechanics0103 physical sciencesMesons (Nuclear physics)Mesons (Física nuclear)010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysicsUnitarityReaccions nuclears010308 nuclear & particles physicsScatteringHigh Energy Physics::PhenomenologyFísicaCromodinàmica quàntica Partícules (Física nuclear)Scattering lengthBaryonPseudoscalarScattering amplitudeHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNuclear reactionsQuantum chromodynamics
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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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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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Determination of the S-wave pion nucleon scattering lengths from πN, pionic hydrogen and deuteron

2005

The isoscalar and isovector scattering lengths ( b 0 , b 1 ) are determined using a unitarized coupled channel approach based on chiral Lagrangians. For the deuterium scattering length a π − d new significant corrections are evaluated, putting new constraints from π − d scattering on the values of ( b 0 , b 1 ) .

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsPionDeuteriumIsovectorScatteringIsoscalarNuclear TheoryS-waveScattering lengthNucleonNuclear Physics A
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Proton-Deuteron Elastic Scattering for E > 0

1999

We report on the first reliable numerical results for proton-deuteron elastic scattering observables for energies above the deuteron breakup thresh- old, for the Paris potential. The calculations have been performed within the screening and renormalisation approach. The theoretical results are compared with recent experimental data.

Nuclear physicsScattering amplitudePhysicsElastic scatteringQuasielastic scatteringPhonon scatteringProtonNuclear TheoryScattering lengthInelastic scatteringNuclear ExperimentBreakup
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Real and Virtual Compton Scattering (experiments)

1999

This paper deals with Real and Virtual Compton Scattering off the proton at threshold and the way to deduce information about the nucleon polarizabilities.

Nuclear physicsScattering cross-sectionPhysicsAnomalous magnetic dipole momentProtonAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryPhysics::Atomic and Molecular ClustersCompton scatteringNuclear ExperimentNucleon
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The relativistic spin-orbit current in deuteron photodisintegration below and above ?-threshold

1988

It is shown that the spin-orbit current which leads to an improved description ofd(γ,p)n below π-threshold is essentially a two-body exchange effect. This is demonstrated by separation of its one-body contribution. Furthermore, above π-threshold its inclusion leads to an improved agreement with experiment, in particular for the differential cross section in the Δ-excitation region.

Nuclear physicsScattering cross-sectionPhysicsCurrent (mathematics)DeuteriumPhotodisintegrationElementary particleOrbit (control theory)Atomic physicsAtomic and Molecular Physics and OpticsSpin-½Few-Body Systems
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High-resolution scattering experiments at the K130 cyclotron in Jyväskylä

2018

Abstract An experimental setup for nuclear reaction studies induced by light and heavy ions is described. It consists of a versatile Large Scattering Chamber equipped with two rotating tables for mounting detectors. A dedicated beam diagnostic system is used to monitor the energy spectrum of the beam on target. The system provides the necessary feedback for tuning of the K-130 cyclotron to reduce the energy spread of the accelerated beam by at least a factor of 3 down to about 0.3% of the nominal energy while maintaining beam currents around 20 pnA. At lower beam currents a 0.1% energy spread can be achieved. This improvement makes a significant impact on the scope of reaction studies possi…

Nuclear reactionNuclear and High Energy PhysicsCyclotronHigh resolution01 natural sciencesIonlaw.inventionscattering experimentsOpticslaw0103 physical sciencessirontacyclotron010306 general physicsInstrumentationPhysicsta114010308 nuclear & particles physicsScatteringbusiness.industrysyklotronitDetectorscattering chamberbeam opticsydinfysiikkabusinessEnergy (signal processing)Beam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The πd scattering length from Kα X-rays

1974

Abstract X-rays from the K α transition (2P → 1S) of the π − d mesic atom have been observed. Their energy, 2592.8 −2.0 +1.6 , has been measured by the critical absorber technique, using the M V absorption edge in bismuth. The strong interaction shift in the 1S state is −4.8 eV, corresponding to a scattering length a ( π d) = −(0.052 −0.017 +0.022 ) m π −1 , in agreement with recent calculations. The intensity ratio K α /K total = 0.548 ± 0.015.

Nuclear reactionPhysicsNuclear and High Energy PhysicsAbsorption edgechemistryAtomStrong interactionchemistry.chemical_elementScattering lengthAtomic physicsIntensity ratioSpectral lineBismuthPhysics Letters B
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