Search results for "Nuclear physic"

showing 10 items of 5307 documents

Ionization efficiency studies with charge breeder and conventional electron cyclotron resonance ion source

2013

Radioactive Ion Beams play an increasingly important role in several European research facility programs such as SPES, SPIRAL1 Upgrade, and SPIRAL2, but even more for those such as EURISOL. Although remarkable advances of ECRIS charge breeders (CBs) have been achieved, further studies are needed to gain insight on the physics of the charge breeding process. The fundamental plasma processes of charge breeders are studied in the frame of the European collaboration project, EMILIE, for optimizing the charge breeding. Important information on the charge breeding can be obtained by conducting similar experiments using the gas mixing and 2-frequency heating techniques with a conventional JYFL 14 …

010302 applied physicsIonizationMaterials scienceta114[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Particle acceleratorCharge (physics)Plasma7. Clean energy01 natural sciencesIon sourceElectron cyclotron resonanceIonlaw.inventionNuclear physicsBreeder (animal)lawIonization0103 physical sciences010306 general physicsInstrumentationComputingMilieux_MISCELLANEOUS
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Positron annihilation characterization of free volume in microand macro-modified Cu0.4Co0.4Ni0.4Mn1.8O4ceramics

2016

Free volume and pore size distribution size in functional micro and macro-micro-modified Cu0.4Co0.4Ni0.4Mn1.8O4 ceramics are characterized by positron annihilation lifetime spectroscopy in comparison with Hg-porosimetry and scanning electron microscopy technique. Positron annihilation results are interpreted in terms of model implication positron trapping and ortho-positronium decaying. It is shown that free volume of positron traps are the same type for macro and micro modified Cu0.4Co0.4Ni0.4Mn1.8O4 ceramics. Classic Tao-Eldrup model in spherical approximation is used to calculation of the size of nanopores smaller than 2 nm using the ortho-positronium lifetime.

010302 applied physicsMaterials sciencePhysics and Astronomy (miscellaneous)Scanning electron microscopeGeneral Physics and Astronomy02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesMolecular physicsCharacterization (materials science)Nuclear physicsNanoporePositronVolume (thermodynamics)visual_art0103 physical sciencesvisual_art.visual_art_mediumCeramicPhysics::Chemical Physics0210 nano-technologyPorositySpectroscopy
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Plasma instabilities of a charge breeder ECRIS

2017

International audience; Experimental observation of plasma instabilities in a charge breeder electron cyclotron resonance ion source (CB-ECRIS) is reported. It is demonstrated that the injection of 133Cs+ or 85Rb+ ion beam into the oxygen discharge of the CB-ECRIS can trigger electron cyclotron instabilities, which restricts the parameter space available for the optimization of the charge breeding efficiency. It is concluded that the transition from a stable to unstable plasma regime is caused by gradual accumulation and ionization of Cs/Rb and simultaneous change of the discharge parameters in 10–100 ms time scale, not by a prompt interaction between the incident ion beam and the ECRIS pla…

010302 applied physicsMaterials science[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Charge (physics)Plasmaplasma instabilitiescharge breederCondensed Matter Physics01 natural sciences010305 fluids & plasmasNuclear physicsBreeder (animal)Physics::Plasma Physics0103 physical sciences
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Conceptual study of a heavy-ion-ERDA spectrometer for energies below 6 MeV

2017

Abstract Elastic recoil detection analysis (ERDA) is a well established technique and it offers unique capabilities in thin film analysis. Simultaneous detection and depth profiling of all elements, including hydrogen, is possible only with time-of-flight ERDA. Bragg ionization chambers or Δ E - E detectors can also be used to identify the recoiling element if sufficiently high energies are used. The chief limitations of time-of-flight ERDA are the beam induced sample damage and the requirement of a relatively large accelerator. In this paper we propose a detector setup, which could be used with 3 MeV to 6 MeV medium heavy beams from either a single ended accelerator (40Ar) or from a tandem…

010302 applied physicsNuclear and High Energy PhysicsERDASpectrometerta114Physics::Instrumentation and DetectorsChemistryDetectortime-of-flight01 natural sciencesNuclear physicsPelletronElastic recoil detectionTime of flightvetyIonizationhydrogen0103 physical sciencesIonization chamber010306 general physicsInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Mechanisms of Electron-Induced Single-Event Upsets in Medical and Experimental Linacs

2018

In this paper, we perform an in-depth analysis of the single-event effects observed during testing at medical electron linacs and an experimental high-energy electron linac. For electron irradiations, the medical linacs are most commonly used due to their availability and flexibility. Whereas previous efforts were made to characterize the cross sections at higher energies, where the nuclear interaction cross section is higher, the focus of this paper is on the complete overview of relevant electron energies. Irradiations at an electron linac were made with two different devices, with a large difference in feature size. The irradiations at an experimental linac were performed with varying en…

010302 applied physicsNuclear and High Energy PhysicsMaterials scienceta114010308 nuclear & particles physicselectronsElectron linacElectronhiukkaskiihdyttimetelektronitparticle accelerators01 natural sciencesLinear particle acceleratorNuclear physicsNuclear interactionradiation physicsCross section (physics)säteilyfysiikkaNuclear Energy and Engineering0103 physical sciencesElectrical and Electronic EngineeringEvent (particle physics)IEEE Transactions on Nuclear Science
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Theoretical and experimental studies of the neutron rich fission product yields at intermediate energies

2012

A new method to measure the fission product independent yields employing the ion guide technique and a Penning trap as a precision mass filter, which allows an unambiguous identification of the nuclides is presented. The method was used to determine the independent yields in the proton-induced fission of 232 Th and 238 U at 25 MeV. The data were analyzed with the consistent model for description of the fission product formation cross section at the projectile energies up to 100 MeV. Pre-compound nucleon emission is described with the two-component exciton model using Monte Carlo method. Decay of excited compound nuclei is treated within time-dependent statistical model with inclusion of the…

010302 applied physicsNuclear fission productCluster decay010308 nuclear & particles physicsFissionChemistryPhysicsQC1-999Nuclear TheoryPenning trap01 natural sciences7. Clean energyNuclear physics0103 physical sciencesNeutronNuclideAtomic physicsNuclear ExperimentNucleonNuclear densityEPJ Web of Conferences
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Commissioning of the vacuum system of the KATRIN Main Spectrometer

2016

The KATRIN experiment will probe the neutrino mass by measuring the β-electron energy spectrum near the endpoint of tritium β-decay. An integral energy analysis will be performed by an electro-static spectrometer (``Main Spectrometer''), an ultra-high vacuum vessel with a length of 23.2 m, a volume of 1240 m[superscript 3], and a complex inner electrode system with about 120 000 individual parts. The strong magnetic field that guides the β-electrons is provided by super-conducting solenoids at both ends of the spectrometer. Its influence on turbo-molecular pumps and vacuum gauges had to be considered. A system consisting of 6 turbo-molecular pumps and 3 km of non-evaporable getter strips ha…

010302 applied physicsPhysicsLight nucleusPhysics - Instrumentation and DetectorsSpectrometerSpectrometersPhysics::Instrumentation and DetectorsVacuum-basedFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)01 natural sciencesEnergy analysisNuclear physics0103 physical sciencesEnergy spectrumGas systems and purificationNeutrino detectorsddc:620010306 general physicsInstrumentationMathematical PhysicsEngineering & allied operationsKATRINdetectors
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Accumulation of positrons from a LINAC based source

2020

International audience; The GBAR experiment aims to measure the gravitational acceleration of antihydrogen H̅. It will use H̅+ ions formed by the interaction of antiprotons with a dense positronium cloud, which will require about 1010 positrons to produce one H̅+. We present the first results on the positron accumulation, reaching 3.8±0.4×108 e+ collected in 560 s.

010302 applied physicsPhysicsMeasure (physics)General Physics and Astronomy02 engineering and technology021001 nanoscience & nanotechnologyGravitational acceleration01 natural sciencesLinear particle acceleratorPositroniumNuclear physicsPositronPositron plasma; Positron accumulation; Antimatter; Penning-Malmberg trap; Greaves-Surko trap; GBAR[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]AntiprotonAntimatter0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Physics::Accelerator PhysicsPhysics::Atomic Physics0210 nano-technologyAntihydrogenComputingMilieux_MISCELLANEOUSActa Physica Polonica A
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Two-neutron correlations at small relative momenta in ^40Ar + ^197Au collisions at 60 MeV/nucleon

2000

Two-neutron correlation functions are measured in the 40Ar + 197Au reaction at 60 MeV/nucleon to study the space-time characteristics of neutron emitting sources. The source temperatures and velocities are deduced by fitting the single-neutron energy spectra with a three-source model. A comparison of the correlation data with the predictions of the model of moving sources and with the dynamical Landau-Vlasov model suggests the relevance of a multisource description. Particular care has been paid to the influence of the relative source abundance on the shape of the correlation function.

010302 applied physicsPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesSpectral lineNuclear physicsCorrelation function (statistical mechanics)0103 physical sciencesnuclear physics; heavy ions; neutron interferometryNeutronNucleonNuclear Experiment
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H− extraction systems for CERN’s Linac4 H− ion source

2018

Abstract Linac4 is a 160 MeV linear H −  accelerator at CERN. It is an essential part of the beam luminosity upgrade of the Large Hadron Collider (LHC) and will be the primary injector into the chain of circular accelerators. It aims at increasing the beam brightness by a factor of 2, when compared to the currently used 50 MeV linear proton accelerator, Linac2. Linac4’s ion source is a cesiated RF-plasma H −  ion source. Several beam extraction systems were designed for H −  beams of 45 keV energy, 50 mA intensity and an electron to H −  ratio smaller than 5. The goal was to extract a beam with an rms-emittance of 0 . 25 π  mm mrad. One of the main challenges in designing an H −  extraction…

010302 applied physicsPhysicsNuclear and High Energy PhysicsLarge Hadron ColliderParticle acceleratorElectron01 natural sciencesIon sourceLinear particle accelerator010305 fluids & plasmasIonlaw.inventionNuclear physicslaw0103 physical sciencesPhysics::Accelerator PhysicsThermal emittanceInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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