Search results for "hadron"

showing 10 items of 3505 documents

The Miniball spectrometer

2013

The Miniball germanium detector array has been operational at the REX (Radioactive ion beam EXperiment) post accelerator at the Isotope Separator On-Line facility ISOLDE at CERN since 2001. During the last decade, a series of successful Coulomb excitation and transfer reaction studies have been performed with this array, utilizing the unique and high-quality radioactive ion beams which are available at ISOLDE. In this article, an overview is given of the technical details of the full Miniball setup, including a description of the γ-ray and particle detectors, beam monitoring devices and methods to deal with beam contamination. The specific timing properties of the REX-ISOLDE facility are hi…

Radioactive ion beamsNuclear and High Energy PhysicsIon beamREX-ISOLDEONLINECoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsSETUPCOULOMB-EXCITATION0103 physical sciencesNuclear fusionSILICON STRIP DETECTOR[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]RELATIVISTIC ENERGIES010306 general physicsNuclear ExperimentNEUTRON KNOCKOUTPhysicsNuclear Physics; Heavy Ions; Hadrons; Particle and Nuclear Physics; Nuclear FusionLarge Hadron ColliderSpectrometerNUCLEI010308 nuclear & particles physicsDetectorRADIOACTIVE ION-BEAMSemiconductor detectorPhysics::Accelerator PhysicsGE DETECTORS
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Analysis methods of safe Coulomb-excitation experiments with radioactive ion beams using the gosia code

2016

With the recent advances in radioactive ion beam technology, Coulomb excitation at safe energies becomes an important experimental tool in nuclear-structure physics. The usefulness of the technique to extract key information on the electromagnetic properties of nuclei has been demonstrated since the 1960's with stable beam and target combinations. New challenges present themselves when studying exotic nuclei with this technique, including dealing with low statistics or number of data points, absolute and relative normalisation of the measured cross sections and a lack of complimentary experimental data, such as excited-state lifetimes and branching ratios. This paper addresses some of these…

Radioactive ion beamsNuclear and High Energy PhysicsIon beamfuusioreaktioCoulomb excitationData analysisFOS: Physical sciencesCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsElectromagnetic moments25.70.De 21.10.Ky; 29.38.Gj 29.85.Fj0103 physical sciencesNuclear Experiment (nucl-ex)particle and nuclear physics010306 general physicsheavy ionsNuclear ExperimentAnalysis methodPhysics010308 nuclear & particles physicsReaccelerated radioactive beams3. Good healthData pointhadronsQuadrupoleydinfysiikka
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The SPEDE spectrometer

2017

8 pags., 10 figs., 2 tabs.

Radioactive ion beamsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsElectron spectrometerPhysics::Instrumentation and DetectorsFOS: Physical sciencesElectronnucl-ex7. Clean energy01 natural sciencesMomentumNuclear physicsInternal conversion0103 physical sciencesNuclear Physics - ExperimentDetectors and Experimental TechniquesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear Experimentphysics.ins-detPhysicsLarge Hadron ColliderSpectrometer010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)Magnetic fieldPhysics::Accelerator Physics
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The upgraded ISOLDE yield database – A new tool to predict beam intensities

2020

At the CERN-ISOLDE facility a variety of radioactive ion beams are available to users of the facility. The number of extractable isotopes estimated from yield database data exceeds 1000 and is still increasing. Due to high demand and scarcity of available beam time, precise experiment planning is required. The yield database stores information about radioactive beam yields and the combination of target material and ion source needed to extract a certain beam along with their respective operating conditions. It allows to investigate the feasibility of an experiment and the estimation of required beamtime. With the increasing demand for ever more exotic beams, needs arise to extend the functi…

Radioactive ion beamsNuclear and High Energy PhysicsYieldsComputer sciencecomputer.software_genre114 Physical sciences01 natural sciencesISOLDEDatabaseFLUKACERN0103 physical sciencesddc:530Production Yield010306 general physicsInstrumentationLarge Hadron ColliderDatabase010308 nuclear & particles physicsIn-target productionYield predictionCross sectionsYield (chemistry)ABRABLAIONIZATIONRelease efficiencycomputerRadioactive beamBeam (structure)Radioactive beamsNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The SPEDE Spectrometer: Combined In-Beam γ-ray and Conversion Electron Spectroscopy with Radioactive Ion Beams

2015

The SPEDE spectrometer [1] aims to combine a silicon detector, for the detection of electrons, with the MINIBALL γ-ray detection array for in-beam studies employing radioactive ion beams at the HIE-ISOLDE facility at CERN. The setup will be primarily used for octupole collectivity [2] and shape coexistence studies [3, 4] in Coulomb excitation experiments. In the shape coexistence cases the transitions between states of the same spin and parity have enhanced E0 strength [5]. Additionally the 0→0 transitions, typically present in nuclei exhibiting shape coexistence [6], can only occur via E0 transitions, i.e. via internal conversion electron emission.

Radioactive ion beamsPhysicsLarge Hadron ColliderSpectrometerta114Physics::Instrumentation and DetectorsParity (physics)Coulomb excitationElectronElectron spectroscopyPhysics::Accelerator PhysicsSilicon detectorAtomic physicsconversion electron spectrometersNuclear Experiment
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"Table 2" of "Measurement of charge asymmetry in hadronic Z decays"

1991

No description provided.

SIN2TWE+ E- --> HADRONSE+ E- ScatteringGAExclusiveGV91.0
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"Table 1" of "Determination of sin**2 theta(w)(eff) using jet charge measurements in hadronic Z decays"

1996

The first sytematic error is due to the experimental uncertainties, whilst the second is due to the uncertainties in the quark charge separations.

SIN2TWHigh Energy Physics::LatticeE+ E- --> HADRONSE+ E- --> Z0E+ E- ScatteringHigh Energy Physics::PhenomenologyExclusiveHigh Energy Physics::Experiment91.2
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"Table 10" of "Energy dependence of event shapes and of alpha(s) at LEP-2."

1999

Moments of the the Total Jet Broadening (BSUM) distributions at cm energies 133, 161, 172 and 183 GeV.

SKEWNESSNAME=BSUMBSUM133.0-183.0Astrophysics::High Energy Astrophysical PhenomenaE+ E- --> HADRONSE+ E- --> JETSE+ E- ScatteringExclusiveHigh Energy Physics::ExperimentJet ProductionVARIANCENAME=BSUMNuclear Experiment
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Measurement ofΥ(1S+2S+3S)production inp+pand Au + Au collisions atsNN=200GeV

2015

Measurements of bottomonium production in heavy-ion and p + p collisions at the Relativistic Heavy Ion Collider (RHIC) are presented. The inclusive yield of the three states, (1S + 2S + 3S), was measured in the PHENIX experiment via electron-positron decay pairs at midrapidity for Au + Au and p + p collisions at root sNN = 200 GeV. The (1S + 2S + 3S) -> e(+)e(-) differential cross section at midrapidity was found to be B(ee)d sigma/dy = 108 +/- 38 (stat) +/- 15 (syst) +/- 11 (luminosity) pb in p + p collisions. The nuclear modification factor in the 30% most central Au + Au collisions indicates a suppression of the total. state yield relative to the extrapolation from p + p collision data. …

Scattering cross-sectionPhysicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsModification factor01 natural sciencesLuminosityNuclear physicsYield (chemistry)0103 physical sciencesHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderPhysical Review C
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<‘γ*N→Δtransition form factors: A new analysis of data onp(e,e′p)π0atQ2=2.8and4.0 (GeV/c)2

2001

Recent JLab data of the differential cross section for the reaction ${p(e,e}^{\ensuremath{'}}p){\ensuremath{\pi}}^{0}$ in the invariant mass region of $1.1lWl1.4 \mathrm{GeV}$ at four-momentum transfer squared ${Q}^{2}=2.8$ and $4.0 (\mathrm{GeV}{/c)}^{2}$ are analyzed with two models, both of which give an excellent description of most of the existing pion electroproduction data below $Wl1.5 \mathrm{GeV}.$ We find that at up to ${Q}^{2}=4.0 (\mathrm{GeV}{/c)}^{2},$ the extracted helicity amplitudes ${A}_{3/2}$ and ${A}_{/2}$ remain comparable with each other, implying that hadronic helicity is not conserved at this range of ${Q}^{2}.$ The ratios ${E}_{1+}{/M}_{1+}$ obtained show, starting …

Scattering cross-sectionPhysicsNuclear and High Energy PhysicsParticle physicsMeson productionPionHadronZero (complex analysis)High Energy Physics::ExperimentInvariant massNuclear ExperimentNuclear theoryHelicityPhysical Review C
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