0000000001314938

AUTHOR

W. Trinder

showing 8 related works from this author

β-decay of 35Ca

1999

Abstract The β-decay of the T z =− 5 2 nucleus 35 Ca was studied at the LISE3 spectrometer at GANIL. The 35 Ca decay scheme was deduced from its β-delayed proton emission into the ground and excited states of 34 Ar and from its β-delayed two-proton emission. The 35 Ca half-life was determined to be 25.7±0.2 ms. The measured transition strength function B(GT) is compared to results obtained from large-scale sd-shell model calculations.

PhysicsNuclear and High Energy PhysicsDecay schemeSpectrometer010308 nuclear & particles physics01 natural sciences7. Clean energymedicine.anatomical_structureTransition strengthExcited state0103 physical sciencesmedicineProton emissionAtomic physics010306 general physicsNucleusPhysics Letters B
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Radioactivity of neutron-rich oxygen fluorine and neon isotopes

1999

The $\ensuremath{\gamma}$ radiation and neutrons emitted following the $\ensuremath{\beta}$ decays of ${}^{24}\mathrm{O},$ ${}^{25--27}\mathrm{F},$ and ${}^{28\ensuremath{-}30}\mathrm{Ne}$ have been measured. The nuclides were produced in the quasifragmentation of a 2.8 GeV ${}^{36}\mathrm{S}$ beam, separated in-flight and identified through time-of-flight and energy-loss measurements. The ions were stopped in a silicon detector telescope, which was used to detect the $\ensuremath{\beta}$ particles emitted in their subsequent radioactive decay. The coincident $\ensuremath{\gamma}$ rays were measured using four large volume germanium detectors mounted close to the implantation point and the …

PhysicsNuclear and High Energy PhysicsIsotopes of germanium010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaGamma ray[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physicsInternal conversionIsotopes of neon13. Climate action0103 physical sciencesBeta particleIsotopes of zirconiumNuclear Experiment010306 general physicsRadioactive decayEnergy (signal processing)
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Few-neutron removal from238U at relativistic energies

1995

As part of a comprehensive study of uranium fragmentation at relativistic energies at the GSI projectile fragment separator, FRS, inclusive neutron-removal cross sections have been measured for severalxn channels at projectile energies of 600 and 950A MeV using targets of Al, Cu and Pb. The variation of the experimental cross sections with target nuclear charge is used to disentangle nuclear and electromagnetic contributions. The electromagnetic cross sections agree surprisingly well with a simple harmonic oscillator calculation of giant dipole resonances based on measured photonuclear cross sections and do not require an extra enhancement of the two-phonon giant dipole excitation as conclu…

PhysicsNuclear and High Energy PhysicsProjectileNuclear Theorychemistry.chemical_elementSimple harmonic motionUraniumEffective nuclear chargeNuclear physicsDipoleFragmentation (mass spectrometry)chemistryNuclear fusionNeutronAtomic physicsNuclear ExperimentNuclear PhysicsZeitschrift für Physik A Hadrons and Nuclei
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First spatial isotopic separation of relativistic uranium projectile fragments

1994

Abstract Spatial isotopic separation of relativistic uranium projectile fragments has been achieved for the first time. The fragments were produced in peripheral nuclear collisions and spatially separated in-flight with the fragment separator FRS at GSI. A two-fold magnetic-rigidity analysis was applied exploiting the atomic energy loss in specially shaped matter placed in the dispersive central focal plane. Systematic investigations with relativistic projectiles ranging from oxygen up to uranium demonstrate that the FRS is a universal and powerful facility for the production and in-flight separation of monoisotopic, exotic secondary beams of all elements up to Z = 92. This achievement has …

Nuclear and High Energy PhysicsTheoryofComputation_COMPUTATIONBYABSTRACTDEVICES010308 nuclear & particles physicsChemistryProjectileNuclear TheoryTheoryofComputation_GENERALSeparator (oil production)chemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]UraniumAccelerators and Storage RingsComputingMethodologies_ARTIFICIALINTELLIGENCE01 natural sciencesNuclear physicsComputingMethodologies_PATTERNRECOGNITIONCardinal point0103 physical sciencesMonoisotopic massAtomic physicsNuclear Experiment010306 general physicsInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Beta-decay of light nuclei close to the proton drip-line: 40Ti and 35Ca

1998

The s-decay of40Ti and35Ca have been studied at the LISE3 spectrometer at GANIL. The decay schemes were deduced from the observed s-delayed proton and γ emission of40Ti and35Ca into the ground and first excited states of39Ca and34Ar, respectively. The Gamow-Teller strength functionB(GT) of the40Ti s-decay extracted from the s-decay branching ratios and the precisely measured40Ti half-life, provides for the first time an experimental calibration of the neutrino detection efficiency for the ICARUS solar neutrino detector.

ICARUSPhysicsDecay schemePhysics::Instrumentation and Detectors010308 nuclear & particles physicsSolar neutrino[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesBeta decayNuclear physicsNeutrino detectorExcited state0103 physical sciencesHigh Energy Physics::ExperimentPositron emissionAtomic physicsProton emissionNuclear Experiment010306 general physicsComputingMilieux_MISCELLANEOUS
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New transitions in the $\beta$-decay of $^{36}$Ca

2001

The β-decay of the Tz = - 2 nucleus 36Ca was studied at the LISE3 magnetic spectrometer at GANIL. Two new proton-emitting states have been detected and the other nine known βp and βγ transitions have been remeasured with improved resolution. A simulation with the GEANT code has been applied to this experimental setup. A comparison with shell model calculations is given.

PhysicsNuclear and High Energy PhysicsSpectrometer010308 nuclear & particles physicsNuclear TheoryResolution (electron density)HadronSHELL model[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsmedicine.anatomical_structure0103 physical sciencesmedicineNuclear fusionAtomic physicsNuclear Experiment010306 general physicsNucleusNuclear Physics
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"Table 2" of "Few neutron removal from U-238 at relativistic energies"

1997

Uranium fragmentation.

inorganic chemicalsU238 CU --> U236 XU238 PB --> U235 XU238 CU --> U235 XU238 PB --> U236 XU238 CU --> U234 XU238 PB --> U234 XIntegrated Cross Sectiontechnology industry and agricultureCross SectionU238 AL --> U236 XSIGcomplex mixturesU238 AL --> U237 XU238 PB --> U237 XU238 CU --> U237 XNUCLEUS NUCLEUS --> U234 XInclusiveU238 AL --> U234 XU238 AL --> U235 XNUCLEUS NUCLEUS --> U237 XNUCLEUS NUCLEUS --> U236 XNUCLEUS NUCLEUS --> U235 X
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"Table 1" of "Few neutron removal from U-238 at relativistic energies"

1997

Uranium fragmentation.

inorganic chemicalsU238 CU --> U236 XU238 CU --> U235 XU238 CU --> U234 XCross Sectioncomplex mixturesU238 CU --> U237 XNUCLEUS NUCLEUS --> U234 XInclusiveNUCLEUS NUCLEUS --> U233 XNUCLEUS NUCLEUS --> U237 XNUCLEUS NUCLEUS --> U236 XNUCLEUS NUCLEUS --> U235 XU238 PB --> U235 XU238 PB --> U236 XU238 PB --> U233 XU238 PB --> U234 XIntegrated Cross Sectiontechnology industry and agricultureU238 AL --> U236 XSIGU238 AL --> U237 XU238 PB --> U237 XU238 AL --> U233 XU238 AL --> U234 XU238 AL --> U235 X
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