Search results for "Accelerator physics"

showing 10 items of 1294 documents

Forward production of charged pions with incident protons on nuclear targets at the CERN Proton Synchrotron

2009

et al.

Nuclear and High Energy PhysicsProtonHadronchemistry.chemical_elementProton Synchrotronddc:500.201 natural sciences7. Clean energyNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear interaction lengthNuclear Experiment010306 general physicsHARPPhysicsLarge Hadron Collider010308 nuclear & particles physicsFísicaSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)chemistryBeamlinePhysics::Accelerator PhysicsHigh Energy Physics::ExperimentBerylliumAtomic physicsParticle Physics - Experiment
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Evidence for Increased neutron and proton excitations between 51−63 Mn

2015

The hyperfine structures of the odd-even 51−63Mnatoms (N=26 −38) were measured using bunched beam collinear laser spectroscopy at ISOLDE, CERN. The extracted spins and magnetic dipole moments have been compared to large-scale shell-model calculations using different model spaces and effective interactions. In the case of 61,63Mn, the results show the increasing importance of neutron excitations across the N=40subshell closure, and of proton excitations across the Z=28shell gap. These measurements provide the first direct proof that proton and neutron excitations across shell gaps are playing an important role in the ground state wave functions of the neutron-rich Mn isotopes. publisher: Els…

Nuclear and High Energy PhysicsProtonNuclear TheoryMagnetic dipole momentsMagnetic dipole momentNuclear Physics - ExperimentNeutronPhysics::Atomic PhysicsNuclear ExperimentWave functionHyperfine structurePhysicsManganeseta114SpinsMagnetic momentMagnetic dipole moment; Manganese; Spin determination; Nuclear and High Energy Physicsmangaanilcsh:QC1-999Spin determinationPhysics::Accelerator PhysicsPräzisionsexperimente - Abteilung BlaumAtomic physicsGround stateMagnetic dipolelcsh:PhysicsPhysics Letters B
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Production and release of ISOL beams from molten fluoride salt targets

2014

In the framework of the Beta Beams project, a molten fluoride target has been proposed for the production of the required 1013 18Ne/s. The production and extraction of such rates are predicted to be possible on a circulating molten salt with 160 MeV proton beams at close to 1 MW power. As a most important step to validate the concept, a prototype has been designed and investigated at CERN-ISOLDE using a static target unit. The target material consisted of a binary fluoride system, NaF:LiF (39:61 mol.%), with melting point at 649 °C. The production of Ne beams has been monitored as a function of the target temperature and proton beam intensity. The prototype development and the results of th…

Nuclear and High Energy PhysicsProtonNuclear engineeringHalideISOL techniqueMETAL TARGETS[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural scienceschemistry.chemical_compoundMolten salt targets0103 physical sciencesMolten saltNuclear Experiment010306 general physicsInstrumentation010302 applied physicsChemistryRadiochemistryAccelerators and Storage RingsBeta (plasma physics)Melting pointPhysics::Accelerator PhysicsFluorideIntensity (heat transfer)Beam (structure)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Demonstration of the double Penning Trap technique with a single proton

2013

Spin flips of a single proton were driven in a Penning trap with a homogeneous magnetic field. For the spin-state analysis the proton was transported into a second Penning trap with a superimposed magnetic bottle, and the continuous Stern-Gerlach effect was applied. This first demonstration of the double Penning trap technique with a single proton suggests that the antiproton magnetic moment measurement can potentially be improved by three orders of magnitude or more. Spin flips of a single proton were driven in a Penning trap with a homogeneous magnetic field. For the spin-state analysis the proton was transported into a second Penning trap with a superimposed magnetic bottle, and the cont…

Nuclear and High Energy PhysicsProtonOrders of magnitude (temperature)Atomic Physics (physics.atom-ph)Other Fields of PhysicsFOS: Physical sciencesGeonium atomPenning traps01 natural sciencesphysics.atom-phPhysics - Atomic Physics010305 fluids & plasmasFundamental symmetries0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic Physics010306 general physicsSpin (physics)Nuclear ExperimentPhysicsPenning trapCPT testsMagnetic fieldAntiprotonPhysics::Accelerator PhysicsIon trapAtomic physicsPhysics Letters B
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Measurement of pion and proton response and longitudinal shower profiles up to 20 nuclear interaction lengths with the ATLAS Tile calorimeter

2010

The response of pions and protons in the energy range of 20–180 GeV, produced at CERN's SPS H8 test-beam line in the ATLAS iron–scintillator Tile hadron calorimeter, has been measured. The test-beam configuration allowed the measurement of the longitudinal shower development for pions and protons up to 20 nuclear interaction lengths. It was found that pions penetrate deeper in the calorimeter than protons. However, protons induce showers that are wider laterally to the direction of the impinging particle. Including the measured total energy response, the pion-to-proton energy ratio and the resolution, all observations are consistent with a higher electromagnetic energy fraction in pion-indu…

Nuclear and High Energy PhysicsProtonTest-beamPion–proton responsePhysics::Instrumentation and DetectorsHadronMonte Carlo methodNuclear TheoryHadronic shower development01 natural sciencesElectromagnetic radiationPartícules (Física nuclear)Nuclear physicsPion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental Techniques010306 general physicsNuclear ExperimentInstrumentationMonte Carlo simulationGEANT4Detectors de radiacióPhysicsCalorimeterLarge Hadron Collider010308 nuclear & particles physicsATLASLongitudinal shower profile for hadronsScintillation counterPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentParametrization
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Measurements of $R^{d}-R^{p}$ and $R^{Ca}-R^{C}$ in deep inelastic muon scattering

1992

Results are presented on the difference in R, the ratio of longitudinally to transversely polarised virtual photon absorption cross sections, for the deuteron and the proton. They are obtained by c ...

Nuclear and High Energy PhysicsProtonmuon nucleus: deep inelastic scatteringNuclear Theorypolarization: longitudinaldeep inelastic scattering: muon deuteronVirtual particlecross section: ratiophoton: absorptionElementary particlemuon deuteron: deep inelastic scattering530Nuclear physicsabsorption: photondeep inelastic scattering: muon ppolarization: transverseHIGH STATISTICS MEASUREMENT; R=SIGMA-L/SIGMA-T; HIGH Q2Nuclear ExperimentAbsorption (electromagnetic radiation)deep inelastic scattering: muon nucleus90: 200: 280 GeVPhysicsHIGH STATISTICS MEASUREMENTMuoncalciumScatteringcarbonstructure function: ratioR=SIGMA-L/SIGMA-TCERN SPSlongitudinal: polarizationParticle scatteringDeuteriummuon p: deep inelastic scatteringHIGH Q2Physics::Accelerator Physicstransverse: polarizationAtomic physicsParticle Physics - Experimentexperimental results
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Reliable extraction of the dB(E1)/dE for 11Be from its breakup at 520 MeV/nucleon

2019

We analyze the breakup of the one-neutron halo nucleus 11Be measured at 520 MeV/nucleon at GSI on Pb and C targets within an eikonal description of the reaction including a proper treatment of special relativity. The Coulomb term of the projectile-target interaction is corrected at first order, while its nuclear part is described at the optical limit approximation. Good agreement with the data is obtained using a description of 11Be, which fits the breakup data of RIKEN. This solves the apparent discrepancy between the dB(E1)/dE estimations from GSI and RIKEN for this nucleus.

Nuclear and High Energy PhysicsRelativistic correctionNuclear TheoryNuclear TheoryFOS: Physical sciencesHalo nucleusSpecial relativityOne-neutron halo nucleidB(E1)/dENuclear breakup01 natural sciencesNuclear physicsNuclear Theory (nucl-th)Eikonal model0103 physical sciencesCoulombmedicineCoulomb breakup010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsEikonal equationBreakupPhysique atomique et nucléairelcsh:QC1-999medicine.anatomical_structureProper treatmentPhysics::Accelerator PhysicsNucleonNucleuslcsh:PhysicsPhysics Letters B
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Scintillation light produced by low-energy beams of highly-charged ions

2007

Measurements have been performed of scintillation light intensities emitted from various inorganic scintillators irradiated with low-energy beams of highly-charged ions from an electron beam ion source (EBIS) and an electron cyclotron resonance ion source (ECRIS). Beams of xenon ions Xe$^{q+}$ with various charge states between $q$=2 and $q$=18 have been used at energies between 5 keV and 17.5 keV per charge generated by the ECRIS. The intensity of the beam was typically varied between 1 and 100 nA. Beams of highly charged residual gas ions have been produced by the EBIS at 4.5 keV per charge and with low intensities down to 100 pA. The scintillator materials used are flat screens of P46 YA…

Nuclear and High Energy PhysicsScintillationPhysics - Instrumentation and DetectorsIon beamChemistryPhysics::Instrumentation and DetectorsAtomic Physics (physics.atom-ph)FOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)ScintillatorIon gunIon sourceIonPhysics - Atomic PhysicsLight intensityIon beam depositionPhysics::Accelerator PhysicsAtomic physicsInstrumentation
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Silicon Detector Telescope for proton detection in electron scattering reactions at MAMI

2012

Abstract A new Silicon Detector Telescope has been constructed and installed within the experimental facility of the A1 collaboration at Mainz Microtron, with the goal to detect low-energy protons. It consists of seven silicon layers for energy and angle measurement and a plastic scintillator for triggering purposes. The detector subtends a solid angle up to 88 msr, depending on the distance from the target and covers the proton kinetic energy range of 25–41  MeV with the mean energy resolution σ E = 0.47 MeV , operating at 500 kHz. Digital signal processing methods applied for energy reconstruction have been important for keeping the acceptable energy resolution at high counting rates. The…

Nuclear and High Energy PhysicsSiliconPhysics::Instrumentation and Detectorschemistry.chemical_elementScintillator01 natural scienceslaw.inventionNuclear physicsTelescopeOpticslaw0103 physical sciencessilicon detector; digital signal processing; electron scatteringNuclear Experiment010306 general physicsInstrumentationMicrotronPhysicsRange (particle radiation)Spectrometer010308 nuclear & particles physicsbusiness.industryDetectorSolid anglechemistryPhysics::Accelerator PhysicsbusinessNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Time-of-flight photoelectron momentum microscopy with 80–500 MHz photon sources: electron-optical pulse picker or bandpass pre-filter

2021

Journal of synchrotron radiation 28(6), 1891 - 1908 (2021). doi:10.1107/S1600577521010511

Nuclear and High Energy PhysicsSpectrum analyzerMaterials sciencePhotonMicroscopephotoelectron diffraction550Synchrotron radiationmomentum microscopylaw.inventionOpticslawddc:550Pulse waveTime domaintime of flight spectroscopy ; momentum microscopy ; ARPES ; photoelectron diffraction ; pulse pickingpulse pickingInstrumentationMomentum (technical analysis)Radiationbusiness.industryARPESResearch PapersTime of flighttime-of-flight spectroscopyPhysics::Accelerator Physicsbusiness
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