Search results for "Accelerator"

showing 10 items of 1507 documents

Half-life ofTi44

1983

The half-life of $^{44}\mathrm{Ti}$ has been measured to be ${T}_{\frac{1}{2}}=54.2\ifmmode\pm\else\textpm\fi{}2.1$ yr, somewhat higher than previously published values of 46.4\ifmmode\pm\else\textpm\fi{}1.7 and 48.2\ifmmode\pm\else\textpm\fi{}0.9 yr. The present value was obtained from the specific activity and the radioisotope concentration of several Ti${\mathrm{O}}_{2}$ samples, each spiked with a $^{44}\mathrm{Ti}$ activity of about 1.2 \ensuremath{\mu}Ci. The specific activity was measured via the 1157 keV $\ensuremath{\gamma}$ line from the decay of the $^{44}\mathrm{Sc}$ daughter. $^{44}\mathrm{Ti}$/Ti concentrations were measured with the Argonne FN tandem accelerator in conjunctio…

PhysicsNuclear and High Energy PhysicsAnalytical chemistryHalf-lifeHeavy ionSensitivity (control systems)Tandem acceleratorAccelerator mass spectrometryPhysical Review C
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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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Instrumentation and optimization studies for a beam dump experiment (BDX) at MESA — DarkMESA

2020

Abstract At the Institute for Nuclear Physics in Mainz the new electron accelerator MESA will go into operation within the next years. The high-power beam dump of the P2 experiment is ideally suited for a parasitic dark sector experiment — DarkMESA. In the first stage 1,000 high density Cherenkov radiators from a previous experiment will be used. The experiment is studied with a simulation based on MadGraph and Geant4 . The simulation includes an optical photon study, where the response of possible calorimeter materials – PbF 2, BGO, the Pb glasses SF5, SF6 and SF57HTultra from Schott – was investigated. The simulation outcomes are compared with the results of prototypes tested at the Mainz…

PhysicsNuclear and High Energy PhysicsCalorimeter (particle physics)010308 nuclear & particles physicsInstrumentationDetectorParticle accelerator01 natural sciencesDark photonlaw.inventionNuclear physicslaw0103 physical sciencesBeam dump010306 general physicsInstrumentationMicrotronCherenkov radiationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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A novel four-quadrant power supply for low-energy correction magnets

2003

Abstract This paper describes an efficient power supply to feed low-energy correction magnets in particle accelerator applications, where a controlled current with trapezoidal profile and four-quadrant operation is needed. The selected design is based on an AC–DC matrix converter topology, which uses the Space Vector Modulation (SVM) technique to obtain a near unity power factor at the AC input and output DC current regulation. This topology allows performing high-frequency isolation, while four-quadrant operation is maintained, and reducing volume and weight as compared with the classical thyristor (SCR)-based technology. Control tasks are implemented on an all-digital control card: output…

PhysicsNuclear and High Energy PhysicsDigital signal processorThyristorParticle acceleratorPower factorQuadrant (instrument)law.inventionSupport vector machinelawMagnetElectronic engineeringInstrumentationSpace vector modulationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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Low energy reactions with radioactive ions at REX-ISOLDE-the 9Li + 2H case

2005

19 pages, 12 figures, 2 tables.-- PACS nrs.: 25.60.-t; 25.45.-z; 27.20.+n.-- et al. ISOLDE Collaborattion and REX-ISOLDE Collaboration.

PhysicsNuclear and High Energy PhysicsExcitation energyC3D6 targetRex-Isolde post-acceleratorIonNuclear physicsLow energyDeduced reaction channelsDeuteriumReaction radioactiveDSSSD detectorAtomic physicsBeam (structure)Radioactive beam
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