Search results for "nuclear physics"

showing 10 items of 5307 documents

The MARA-LEB ion transport system

2020

Abstract A low-energy branch is under development for the MARA vacuum-mode recoil separator at the Accelerator Laboratory of the University of Jyvaskyla. This development will allow for the study of proton-rich nuclei through laser ionisation spectroscopy and mass measurements. After stopping and extraction from a buffer gas cell, the ions of interest will be accelerated and transported to dedicated experimental setups by an ion transport system consisting of several focusing, accelerating and mass-separating elements. This article presents the current design and simulations for the ion transport.

Nuclear and High Energy PhysicsMaterials scienceBuffer gasLaser01 natural sciencesRecoil separatorlaw.inventionIonNuclear physicslawIonization0103 physical sciencesCurrent (fluid)Nuclear Experiment010306 general physicsSpectroscopy010303 astronomy & astrophysicsInstrumentationIon transporterNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Onset of deformation in neutron-rich krypton isotopes

1988

Beta-decay properties of neutron-rich35Br isotopes confirm the predicted smooth onset of quadrupole deformation for Z<37 already below N=60. The observed increase of the energy of the first 2+ state in the N=56 nucleus92Kr may indicate octupole softness.

Nuclear and High Energy PhysicsMaterials scienceIsotopeNuclear TheoryKryptonIsotopes of kryptonchemistry.chemical_elementElementary particleDeformation (meteorology)chemistryQuadrupoleNuclear fusionNuclear Physics - ExperimentNeutronPhysics::Atomic PhysicsAtomic physicsZeitschrift f�r Physik A Atomic Nuclei
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Thermo-mechanical testing of Li-ceramic for the helium cooled pebble bed (HCPB) breeding blanket

2004

The helium cooled pebble bed (HCPB) Test blanket module (TBM) for the DEMO Reactor foresees the utilization of lithiate ceramics as breeder in form of pebble beds. The pebbles are organized in several layers alternatively stacked among couples of cooling plates (CP). ENEA has launched an experimental programme for the out-of-pile thermo-mechanical testing of mock-ups simulating a portion of the HCPB-TBM. The programme foresees the fabrication and testing of different mock-ups, to be tested in the HE-FUS3 facility at ENEA Brasimone. The paper describes the HELICHETTA III campaign carried-out in 2003. In particular, the test section layout, the pebble filling procedure, the experimental set-u…

Nuclear and High Energy PhysicsMaterials scienceNuclear engineeringFUSION REACTOR BREEDING BLANKET PEBBLE BEDSchemistry.chemical_elementBlanketNuclear physicsBreeder (animal)Nuclear Energy and Engineeringchemistryvisual_artvisual_art.visual_art_mediumGeneral Materials ScienceCeramicPebbleHeliumThermo mechanicalSettore ING-IND/19 - Impianti Nucleari
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Tritium retention measurements by accelerator mass spectrometry and full combustion of W-coated and uncoated CFC tiles from the JET divertor

2016

Abstract Accelerator mass spectrometry (AMS) and the full combustion method (FCM) followed by liquid scintillation counting were applied to quantitatively determine the tritium retention in the tungsten-coated carbon fibre composites (CFC), in comparison to uncoated CFC tiles from the JET divertor. The tiles were adjacent and exposed to plasma operations between 2007 and 2009. The tritium depth profiles are showing that the tritium retention on the W-coated tile was reduced by a factor of 13.5 in comparison to the uncoated tile whereas the bulk tritium concentration is approximately the same for both tiles.

Nuclear and High Energy PhysicsMaterials scienceanimal structuresgenetic structuresgenetic processesCombustion01 natural sciences010305 fluids & plasmasNuclear physicstritium retention0103 physical sciencesnatural sciencesdivertor tiles010302 applied physicsJet (fluid)DivertorRadiochemistryLiquid scintillation countingPlasmaCondensed Matter PhysicsJETsurface and bulk distributionvisual_artvisual_art.visual_art_mediumTritiumTilesense organsAccelerator mass spectrometry
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Heavy-Ion Microbeam Studies of Single-Event Leakage Current Mechanism in SiC VD-MOSFETs

2020

Heavy-ion microbeams are employed for probing the radiation-sensitive regions in commercial silicon carbide (SiC) vertical double-diffused power (VD)-MOSFETs with micrometer accuracy. By scanning the beam spot over the die, a spatial periodicity was observed in the leakage current degradation, reflecting the striped structure of the power MOSFET investigated. Two different mechanisms were observed for degradation. At low drain bias (gate and source grounded), only the gate-oxide (at the JFET or neck region) is contributing in the ion-induced leakage current. For exposures at drain–source bias voltages higher than a specific threshold, additional higher drain leakage current is observed in t…

Nuclear and High Energy PhysicsMaterials sciencemicrobeamsilicon carbide (SiC) vertical double-diffused power(VD)-MOSFETleakage current degradation01 natural sciencesDie (integrated circuit)chemistry.chemical_compoundpuolijohteet0103 physical sciencesMOSFETSilicon carbideNuclear Physics - ExperimentPower semiconductor deviceElectrical and Electronic EngineeringPower MOSFETsingle-event effect (SEE)010308 nuclear & particles physicsbusiness.industryionisoiva säteilyHeavy ion; leakage current degradation; microbeam; silicon carbide (SiC) vertical double-diffused power(VD)-MOSFET; single-event effect (SEE); single-event leakage current (SELC)JFETSELCMicrobeamSiC VD-MOSFET620single event effectsäteilyfysiikkaNuclear Energy and Engineeringchemistryheavy-ionOptoelectronicsddc:620Heavy ionbusinesssingle-event leakage current (SELC)Voltage
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Measurement of the spin density matrix for the rho(0), K*(0)(892) and phi produced in Z(0) decays

1997

The spin density matrix elements for the rho(0), K-*0(892) and phi produced in hadronic Z(0) decays are measured in the DELPHI detector. There is no evidence for spin alignment of the K-*0(892) and phi, in the region x(p) less than or equal to 0.3 (x(p) = p/p(beam)), where rho(00) = 0.33 +/- 0.05 and rho(00) = 0.30 +/- 0.04, respectively. In the fragmentation region, x(p) greater than or equal to 0.4, there is some indication for spin alignment of the rho(0) and K-*0(892), since rho(00) = 0.43 +/- 0.05 and rho(00) = 0.46 +/- 0.08, respectively. These values are compared with those found in meson-induced hadronic reactions. For the phi, rho(00) = 0.30 +/- 0.04 for x(p) greater than or equal …

Nuclear and High Energy PhysicsMesonElectron–positron annihilationD-STARHadronANNIHILATIONSPartícules (Física nuclear)QUARK FRAGMENTATION; D-STAR; ANNIHILATIONS; HADRONS; MESONSNuclear physicsAngular distribution[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Matrix elementSpin densityDetectors de radiacióDELPHIPhysicsHADRONSD-STARQUARK FRAGMENTATIONLARGE ELECTRON POSITRON COLLIDERMESONSPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIMass spectrumPARTICLE PHYSICSAtomic physicsParticle Physics - ExperimentPHYSICS LETTERS B
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Experimental program of the Super-FRS Collaboration at FAIR and developments of related instrumentation

2016

The physics program at the super-conducting fragment separator (Super-FRS) at FAIR, being operated in a multiple-stage, high-resolution spectrometer mode, is discussed. The Super-FRS will produce, separate and transport radioactive beams at high energies up to 1.5 AGeV, and it can be also used as a stand-alone experimental device together with ancillary detectors. Various combinations of the magnetic sections of the Super-FRS can be operated in dispersive, achromatic or dispersion-matched spectrometer ion-optical modes, which allow measurements of momentum distributions of secondary-reaction products with high resolution and precision. A number of unique experiments in atomic, nuclear and h…

Nuclear and High Energy PhysicsMesonNeutron emissionCOHERENT EXCITATIONProjectile fragments01 natural sciences114 Physical scienceslaw.inventionNuclear physicsENERGYlaw0103 physical sciencesSCATTERINGSPECTROMETERFACILITY010306 general physicsSpectroscopyNuclear ExperimentInstrumentationPhysicsta114IsotopeSpectrometerNUCLEI010308 nuclear & particles physicsScatteringDetectorMagnetic spectrometerPERFORMANCEINVERSE KINEMATICSPRODUCTSSTATESAchromatic lensExperiments
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Large-angle production of charged pions with 3-12.9 GeV/c incident protons on nuclear targets

2008

Measurements of the double-differential pi(+/-) production cross section in the momentum range 100 <= p <= 800 MeV/c and angle range 0.35 <= theta <= 2.15 rad in proton-beryllium, proton-carbon, proton-aluminium, proton-copper, proton-tin, proton-tantalum, and proton-lead collisions are presented. The data were taken with the large-acceptance HARP detector in the T9 beam line of the CERN PS. The pions were produced by proton beams in a momentum range from 3 to 12.9 GeV/c hitting a target with a thickness of 5% of a nuclear interaction length. Tracking and identification of the produced particles was performed by using a small-radius cylindrical Time Projection Chamber (TPC) placed inside a …

Nuclear and High Energy PhysicsMesonProtonPhysics::Instrumentation and DetectorsHadronNuclear TheoryFOS: Physical sciencesddc:500.27. Clean energy01 natural sciencesParticle detectorHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear interaction length010306 general physicsNuclear ExperimentPhysicsTime projection chamber010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleFísicaCharged particlePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentAtomic physicsNucleonParticle Physics - Experiment
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Measurement of the ratioB(B+→Xeν)/B(B0→Xeν)

2005

We report measurements of the inclusive electron momentum spectra in decays of charged and neutral B mesons, and of the ratio of semileptonic branching fractions B(B+-> Xe nu) and B(B-0 -> Xe nu). These were performed on a sample of 231x10(6) B (B) over bar events recorded with the BABAR detector at the Upsilon(4S) resonance. Events are selected by fully reconstructing a hadronic decay of one B meson and identifying an electron among the decay products of the recoiling (B) over bar meson. We obtain B(B+-> Xe nu)/B(B-0 -> Xe nu)=1.074 +/- 0.041((stat))+/- 0.026((syst)).

Nuclear and High Energy PhysicsMesonmedia_common.quotation_subjectElectron–positron annihilationHadronElementary particleElectronAsymmetry01 natural sciencesNuclear physicsParticle decayTheoretical physicsTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesB mesonNuclear Experiment010306 general physicsmedia_commonBosonPhysicsBranching fraction010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCrystallographyHigh Energy Physics::ExperimentLeptonPhysical Review D
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Muon Knight shift at a structural defect in zinc crystals

1984

The interaction of a light hydrogen isotope with a structural defect is traced for the first time by means of the temperature dependence of the muon Knight shiftKμ in the hcp metal Zn. A surprising result is the huge and negativeKμ (−520 ppm) at the defect site, probably a multivacancy cluster.

Nuclear and High Energy PhysicsMuonCondensed matter physicsIsotopechemistry.chemical_elementKnight shiftZincCondensed Matter PhysicsAtomic and Molecular Physics and OpticsLight hydrogenNuclear physicsMetalchemistryvisual_artCluster (physics)visual_art.visual_art_mediumPhysical and Theoretical ChemistryHyperfine Interactions
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