Search results for "Physics::Accelerator Physics"

showing 10 items of 1235 documents

Detector response of Cherenkov radiators for calorimetry in the energy range below 14 MeV

2020

Abstract A study of the detector response of PbF 2  crystals and three different types of lead glass blocks to electrons from a 14-MeV beam of the Mainz Microtron MAMI is presented. For the first time, signal height, signal width, and homogeneity of the response of these Cherenkov radiators were determined for energies between 10 and 14 MeV. To complement the beam tests, optical properties of the materials, in particular measured transmittances in the near UV and visible spectrum, were studied. The measured detector responses were also compared to Monte Carlo simulations of energy-loss, light production, transport, and detection. These Cherenkov radiators are considered as active material o…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsbusiness.industryDetectorMonte Carlo methodSignal WidthElectron01 natural sciencesLead glassOpticsvisual_art0103 physical sciencesvisual_art.visual_art_mediumPhysics::Accelerator PhysicsNuclear Experiment010306 general physicsbusinessInstrumentationLight dark matterMicrotronCherenkov radiationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The effect of magnetic field strength on the time evolution of high energy bremsstrahlung radiation created by an electron cyclotron resonance ion so…

2009

Abstract An electron cyclotron resonance (ECR) ion source is one of the most used ion source types for high charge state heavy ion production. In ECR plasma the electrons are heated by radio frequency microwaves in order to provide ionization of neutral gases. As a consequence, ECR heating also generates very high electron energies (up to MeV region) which can produce a vast amount of bremsstrahlung radiation causing problems with radiation shielding and heating superconducting cryostat of an ECR ion source. To gain information about the time evolution of the electron energies in ECR plasma radial bremsstrahlung measurements were performed. JYFL 14 GHz ECR ion source was operated in pulsed …

PhysicsNuclear and High Energy PhysicsArgonBremsstrahlungchemistry.chemical_elementPlasmaElectronElectron cyclotron resonanceIon sourcechemistryPhysics::Plasma PhysicsIonizationPhysics::Accelerator PhysicsAtomic physicsInstrumentationIon cyclotron resonanceNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Measurements of charge state distributions of 0.74 and 1.4  MeV/u heavy ions passing through dilute gases

2017

In many modern heavy-ion accelerator facilities, gas strippers are used to increase the projectile charge state for improving the acceleration efficiency of ion beams to higher energies. For this application, the knowledge on the behavior of charge state distributions of heavy-ions after passing through dilute gases is of special interest. Charge state distributions of uranium ($^{238}\mathrm{U}$), bismuth ($^{209}\mathrm{Bi}$), titanium ($^{50}\mathrm{Ti}$), and argon ($^{40}\mathrm{Ar}$) ion beams with energies of $0.74\text{ }\mathrm{MeV}/\mathrm{u}$ and $1.4\text{ }\mathrm{MeV}/\mathrm{u}$ after passing through hydrogen (${\mathrm{H}}_{2}$), helium (He), carbon dioxide (${\mathrm{CO}}_{…

PhysicsNuclear and High Energy PhysicsArgonPhysics and Astronomy (miscellaneous)Hydrogen010308 nuclear & particles physicschemistry.chemical_elementCharge (physics)Surfaces and Interfaces010403 inorganic & nuclear chemistry01 natural sciences0104 chemical sciencesBismuthIonNeonchemistry0103 physical sciencesPhysics::Accelerator PhysicsProduction (computer science)Atomic physicsHeliumPhysical Review Accelerators and Beams
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Production of neutron-rich isotopes in fission of uranium induced by neutrons of 20 MeV average energy

2000

In the context of a parameter study conducted by several laboratories for future European radioactive beam facilities based on fast-neutron induced fission, in particular for the SPIRAL-II project at GANIL, we have measured the yields of neutron-rich isotopes in the mass range of 88 to 144. These nuclei were obtained as fission products of natural uranium bombarded by neutrons of 20 MeV average energy emitted by a thick carbon target irradiated by 50 MeV deuterons. Yields have been measured using on-line mass separation with the ion-guide method. Compared with proton-induced fission at 25 MeV the magnitude of cross-sections, except for the symmetric region, is similar. Z-distributions of is…

PhysicsNuclear and High Energy PhysicsCold fissionIsotopes of uranium010308 nuclear & particles physicsNeutron emissionIsotopes of samariumNuclear TheoryFission product yield[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyFast fissionNuclear physicsUranium-2380103 physical sciencesPhysics::Accelerator PhysicsNuclear Experiment010306 general physicsLong-lived fission product
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The polarized double cell target of the SMC

1999

The polarized target of the Spin Muon Collaboration at CERN was used for deep inelastic muon scattering experiments during 1993-1996 with a polarized muon beam to investigate the spin structure of the nucleon. Most of the experiments were carried out with longitudinal target polarization and 190 GeV muons, and some were done with transverse polarization and 100 GeV muons. Protons as well as deuterons were polarized by dynamic nuclear polarization (DNP) in three kinds of solid materials - butanol, ammonia, and deuterated butanol - with maximum degrees of polarization of 94%, 91% and 60%, respectively. Considerable attention was paid to the accuracies of the NMR polarization measurements and …

PhysicsNuclear and High Energy PhysicsDISLarge Hadron ColliderMuonanalysisScatteringSMCPolarized targetSpin structurepolarized protons and deuteronsPolarization (waves)Deep inelastic scatteringNMRdynamic nuclear polarizationSMC; DIS; Polarized targetNuclear physicsDeuteriumPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentDetectors and Experimental TechniquesNuclear ExperimentNucleonInstrumentation
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Decay properties of neutron deficient Kr isotopes

1974

The decay properties of the neutron deficient isotopes73–77Kr and73–76Br have been studied at the ISOLDE facility at CERN. The total decay energiesQ, as determined fromβ + singles orβ + -γ coincidence measurements, are compared with mass formulae.

PhysicsNuclear and High Energy PhysicsDecay schemeIsotopes of germaniumBeta-decay stable isobarsNuclear physicsIsotopes of protactiniumBeta particlePhysics::Accelerator PhysicsIsotopes of zirconiumHigh Energy Physics::ExperimentNeutronAlpha decayNuclear ExperimentZeitschrift für Physik
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The 1.5GeV harmonic double-sided microtron at Mainz University

2008

Abstract At the Institut fur Kernphysik of Mainz University a harmonic double-sided microtron (HDSM) has been built to extend the experimental capabilities for nuclear and particle physics experiments to higher excitation energies. This novel microtron variant accelerates the 0.855 GeV continuous wave (cw) electron beam of the established three-staged race track microtron (RTM) cascade MAMI B up to 1.5 GeV. It consists of two normal conducting linear accelerators (linacs) through which the electrons are guided up to 43 times by a pair of 90°-bending magnets at each end. For beam dynamical reasons the linacs operate at the harmonic frequencies of 4.90 and 2.45 GHz. The extended facility is c…

PhysicsNuclear and High Energy PhysicsElectronLinear particle acceleratorNuclear physicsAccelerationCathode rayHarmonicPhysics::Accelerator PhysicsNuclear ExperimentInstrumentationMicrotronBeam (structure)ExcitationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A hot cavity laser ion source at IGISOL

2008

A development program is underway at the IGISOL (Ion Guide Isotope Separator On-Line) facility, University of Jyvaskyla, to efficiently and selectively produce low-energy radioactive ion beams of silver isotopes and isomers, with a particular interest in N=Z 94Ag. A hot cavity ion source has been installed, based on the FEBIAD (Forced Electron Beam Induced Arc Discharge) technique, combined with a titanium:sapphire laser system for selective laser ionization. The silver recoils produced via the heavy-ion fusion-evaporation reaction, 40Ca(58Ni, p3n)94Ag, are stopped in a graphite catcher, diffused, extracted and subsequently ionized using a three-step laser ionization scheme. The performance…

PhysicsNuclear and High Energy PhysicsFOS: Physical sciencesPhysics::OpticsLaserIon sourceIonlaw.inventionElectric arclawIonizationPhysics::Atomic and Molecular ClustersSapphireCathode rayPhysics::Accelerator PhysicsPhysics::Atomic PhysicsGraphiteNuclear Experiment (nucl-ex)Atomic physicsNuclear ExperimentNuclear ExperimentThe European Physical Journal A
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Positron implantation profiles in layered samples

2009

The paper presents theoretical and experimental studies of the positron implantation profiles in layered samples. The Monte Carlo simulations performed using the GEANT4 toolkit reveal accumulation of positrons in the denser layer embedded between two less dense layers. That effect is significant not only for low energy positrons at slow monoenergetic positron beams but also for high energy positrons which are emitted from radioactive nuclei in conventional experiments. Measurements of the positron implantation profile into the samples which consist of silver and aluminium foils of different thickness show profile features which correspond well with those simulated by the GEANT4 toolkit for …

PhysicsNuclear and High Energy PhysicsHigh energyAstrophysics::High Energy Astrophysical PhenomenaPositron Lifetime SpectroscopyPhysics::Medical PhysicsMonte Carlo methodchemistry.chemical_elementLow energyPositronchemistryAluminiumPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentAtomic physicsInstrumentationLayer (electronics)Positron annihilationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Electro-produced slow positrons

1989

During the last 6 years it has been demonstrated that electro-produced intense beams of slow positrons are possible. High energy electrons from an accelerator generate bremsstrahlung in a thick conversion target of high element number Z. The photons produce electronpositron pairs and a small fraction of the positrons may be moderated to thermal energies. A review is given of the existing slow positron beam lines using this technique. At accelerator energies of 100 MeV total conversion efficiencies of several slow positrons per 106 primary electrons have been obtained, resulting in average intensities of several 109 slow positrons per second or more than 105 slow positrons in pulses having a…

PhysicsNuclear and High Energy PhysicsHigh energyPhotonBremsstrahlungElectronCondensed Matter PhysicsAtomic and Molecular Physics and OpticsIntensity (physics)Nuclear physicsPositronThermalPhysics::Accelerator PhysicsPhysical and Theoretical ChemistryAtomic physicsOrder of magnitudeHyperfine Interactions
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