Search results for "beam"

showing 10 items of 2126 documents

Invariant mass spectrum and α-n correlation function studied in the fragmentation of 6He on a carbon target

1998

13 pags, 5 figures.-- PACS nrs.: 24.60.−t; 25.70.Ef; 27.20.+n.

PhysicsNuclear and High Energy PhysicsReaction mechanismMomentum distributionsBreakupSpectral lineIon[PACS] Reactions induced by unstable nucleiBreakup reactions6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)Halo nucleiFragmentation mechanism[PACS] ResonancesSecondary radioactive beamsInvariant massNeutronHe-5He-6Invariant mass spectra[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physicsGround stateExotic nucleiNuclear Physics A
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Transverse laser cooling of a radio-frequency bunched ion beam in the storage ring TSR

1996

Abstract We report on the observation of the indirect transverse laser cooling effect in a radio-frequency bunched beam of 7.3 MeV 9 Be + ions, stored in the Heidelberg Test Storage Ring and subject to direct longitudinal laser cooling. This bunched scheme offers particular advantages for producing ultracold beams with unprecedented phase-space densities.

PhysicsNuclear and High Energy PhysicsResolved sideband coolingIon beamIonTransverse planeLaser coolingPhysics::Accelerator PhysicsPhysics::Atomic PhysicsRadio frequencyAtomic physicsNuclear ExperimentInstrumentationBeam (structure)Storage ring
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THE COMPTON BACKSCATTERING POLARIMETER OF THE A4 EXPERIMENT

2005

Abstract The A4 collaboration at the Institut fur Kernphysik, University of Mainz, is conducting experiments on single-spin asymmetries in the elastic electron–nucleon-scattering which require polarized beams. In order to measure the absolute beam polarization, we have installed a Compton backscattering polarimeter in front of the target, using for the first time the internal cavity concept. A maximum intra-cavity intensity of 90 W has been measured, and in August 2003, first backscattered photons have been detected. Recently, first Compton asymmetries have been measured.

PhysicsNuclear and High Energy PhysicsResonatorPhotonOpticsInternal cavitybusiness.industryMeasure (physics)Physics::Accelerator PhysicsBeam polarizationPolarimeterbusinessCompton backscatteringSpin 2004
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Tests of the Standard Model with Low-Energy Neutrino Beams

2007

We discuss the possibility of using future high--intensity low--energy neutrino beams for precision tests of the Standard Model. In particular we consider the determination of the electroweak mixing angle from elastic and quasi--elastic neutrino--nucleon scattering at a superbeam or $\beta$--beam.

PhysicsNuclear and High Energy PhysicsScatteringElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesAtomic and Molecular Physics and OpticsSettore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciStandard ModelNuclear physicsHigh Energy Physics - PhenomenologyLow energyHigh Energy Physics - Phenomenology (hep-ph)Physics::Accelerator PhysicsHigh Energy Physics::ExperimentNeutrinoMixing (physics)Beam (structure)
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A dedicated decay-spectroscopy station for the collinear resonance ionization experiment at ISOLDE

2013

A newdecay-spectroscopystation(DSS)has been developed to be coupled to the collinear resonance ionization spectroscopy (CRIS) beam line at CERN-ISOLDE. The system uses a rotatable wheel with ten 20 mg=cm2 carbon foils as beam implantation sites for the efficient measurement of charged decay products. Silicon detectors are placed on either side of the carbon foil in an optimal geometry to cover a large solid angle for detecting these charged particles. In addition to the silicon detectors at the on-beam axis position, a second pair of off-beam axis detectors are placed at the wheel position 108 deg. away, allowing longer-lived species to be studied. Up to three high purity germanium detector…

PhysicsNuclear and High Energy PhysicsSilicon010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsUltra-high vacuumGamma raychemistry.chemical_elementGermaniumFission products[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesCharged particleBeamlinechemistry0103 physical sciencesPhysics::Accelerator PhysicsAlpha decaygamma-rayAtomic physics010306 general physicsSpectroscopyLaser-assisted decay spectroscopyInstrumentationBeam (structure)
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New gas-filled mode of the large-acceptance spectrometer VAMOS

2010

A new gas-filled operation mode of the large-acceptance spectrometer VAMOS at GANIL is reported. A beam rejection factor greater than 10(10) is obtained for the Ca-40+Sm-150 system at 196 MeV. The unprecedented transmission efficiency for the evaporation residues produced in this reaction is estimated to be around 80% for alpha x n channels and above 95% for x ny p channels. A detailed study of the performance of the gas-filled VAMOS and future developments are discussed. This new operation mode opens avenues to explore the potential of fusion reactions in various kinematics. (C) 2010 Elsevier B.V. All rights reserved.

PhysicsNuclear and High Energy PhysicsSpectrometer010308 nuclear & particles physicsGas-filled spectrometerMode (statistics)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesNuclear physicsNuclear magnetic resonanceOperation mode0103 physical sciencesBeam rejectionNuclear fusionTransmission[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsInstrumentationBeam (structure)Fusion reactions
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Study of $^{45}$Ar through (d, p) reaction at SPIRAL

2005

NESTER; International audience; The structure of the neutron-rich nucleus $^{45}$Ar has been investigated through the d($^{44}$Ar,$^{45}$Ar)p transfer reaction. Radioactive beam of $^{44}$Ar at 10 A MeV has been provided by the SPIRAL facility at GANIL. The protons corresponding to a neutron pick-up on bound or unbound states mechanism in $^{45}$Ar nuclei were detected at backward angles by the detector array MUST. The transfer-like ejectiles were detected in the SPEG spectrometer. Level scheme, spin assignments and spectroscopic factors have been deduced for $^{45}$Ar and compared to shell model predictions. These parameters will be subsequently used to infer (n, $\gamma$) cross sections i…

PhysicsNuclear and High Energy PhysicsSpectrometer010308 nuclear & particles physicsSHELL modelNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physicsmedicine.anatomical_structure0103 physical sciencesPhysics::Space PhysicsmedicineAstrophysics::Solar and Stellar AstrophysicsNeutronAtomic physicsDetector array010306 general physicsSpin (physics)Nuclear ExperimentNucleusRadioactive beamSpiral
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High-resolution study ofTz=+2→+1Gamow-Teller transitions in the44Ca(3He,t)44Sc reaction

2013

PhysicsNuclear and High Energy PhysicsSpectrometer010308 nuclear & particles physicsScatteringHigh resolution01 natural sciencesBeta decayBeamlineDouble beta decay0103 physical sciencesAtomic physics010306 general physicsExcitationPhysical Review C
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Triple GEM tracking detectors for COMPASS

2002

The small area tracker of COMPASS, a high-luminosity fixed target experiment at CERN's SPS, includes a set of 20 large-size ($31\times 31\,\cm^2$) Gas Electron Multiplier (GEM) detectors. Based on gas amplification in three cascaded GEM foils, these devices permit to obtain high gain and good spatial resolution even at very high particle fluxes. A two-coordinate projective readout yields, for each track, highly correlated signal amplitudes on both projections, allowing to resolve multiple hits in high occupancy regions close to the central deactivated area of $5\,\cm$ diameter. At the same time the material exposed to the beam is minimized. Splitting the amplification in three cascaded stag…

PhysicsNuclear and High Energy PhysicsSpectrometerPhysics::Instrumentation and Detectorsbusiness.industryDetectorTracking (particle physics)Nuclear physicsOpticsNuclear Energy and EngineeringCompassNuclear electronicsGas electron multiplierDetectors and Experimental TechniquesElectrical and Electronic EngineeringbusinessImage resolutionBeam (structure)IEEE Transactions on Nuclear Science
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Measuring the proton spectrum in neutron decay - latest results with aSPECT

2008

The retardation spectrometer aSPECT was built to measure the shape of the proton spectrum in free neutron decay with high precision. This allows us to determine the antineutrino electron angular correlation coefficient a. We aim for a precision more than one order of magnitude better than the present best value, which is Delta_a /a = 5%. In a recent beam time performed at the Institut Laue-Langevin during April / May 2008 we reached a statistical accuracy of about 2% per 24 hours measurement time. Several systematic effects were investigated experimentally. We expect the total relative uncertainty to be well below 5%.

PhysicsNuclear and High Energy PhysicsSpectrometerProtonCabibbo–Kobayashi–Maskawa matrixFOS: Physical sciencesElectronMeasure (mathematics)Nuclear physicsNeutronNuclear Experiment (nucl-ex)Nuclear ExperimentInstrumentationNuclear ExperimentOrder of magnitudeBeam (structure)
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