Search results for "Intensity"

showing 10 items of 1091 documents

Precision measurement of the half-life and the decay branches of 62Ga

2005

In an experiment performed at the Accelerator Laboratory of the University of Jyvaskyla, the beta-decay half-life of 62Ga has been studied with high precision using the IGISOL technique. A half-life of T1/2 = 116.09(17)ms was measured. Using beta-gamma coincidences, the gamma intensity of the 954keV transition and an upper limit of the beta-decay feeding of the 0+_2 state have been extracted. The present experimental results are compared to previous measurements and their impact on our understanding of the weak interaction is discussed.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsIGISOL TECHNIQUEHalf-lifeFOS: Physical sciencesState (functional analysis)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Weak interaction01 natural sciencesIntensity (physics)Nuclear physics23.40.-s $\beta$ decay ; double $\beta$ decay ; electron and muon capture - 21.10. Tg Lifetimes - 27.50.+e 59 < A < 890103 physical sciencesLimit (mathematics)Nuclear Experiment (nucl-ex)010306 general physicsNuclear Experiment
researchProduct

On the decay of theJπ= 11/2−,T1/2= 38.9 h isomer in133Ba: search for the E5 transition and verification of the EC branch

2010

International audience; This paper presents a search for the competing 11/2 − → 1/2 + E5 branch to the main 11/2 − → 3/2 + M4 transition from the T 1/2 = 39 h, J π = 11/2 − isomeric state in 133 Ba. An upper limit of 1.8 * 10 −5 could be established for the E5/M4 intensity ratio. In addition a long-standing controversy in the EC-decay of the same isomer was resolved: only one EC branch to the 11/2 + state in 133 Cs was observed. The shell-model structures of the involved states in 133 Ba and 133 Cs were studied with the microscopic quasiparticle-phonon model (MQPM). Good agreement with the decay rates B(λ) was obtained. In particular, the B(M4) value is well reproduced and further only one …

PhysicsNuclear and High Energy Physics21.60.-n010308 nuclear & particles physicsState (functional analysis)Intensity ratio01 natural sciences23.40.-s23.35.+g21.60.Cs0103 physical sciences23.20.-gNuclideAtomic physics010306 general physicsJournal of Physics G: Nuclear and Particle Physics
researchProduct

Single-step link from yrast SD band in 143Eu

1997

A discrete γ-ray transition from the yrast SD band to the region of near-yrast discrete normal-deformed states has been identified in 143Eu. It has an energy of 3360.6 keV and an intensity corresponding to 3.2% of the full intensity of the SD band and feeds a nearly-spherical state above spin 352(+) and Ex=4947 keV. This agrees well with the picture of the decay out of the SD band gained previously from two-step links. The angular distribution analysis favours a stretched dipole character for the transition. Due to the complicated structure of the level scheme in the region of interest it has not been possible to place the transition exactly.

PhysicsNuclear and High Energy PhysicsDipoleAngular distributionYrastSingle stepLink (geometry)Atomic physicsSpin-½Intensity (physics)Progress in Particle and Nuclear Physics
researchProduct

Electro-produced slow positrons

1989

During the last 6 years it has been demonstrated that electro-produced intense beams of slow positrons are possible. High energy electrons from an accelerator generate bremsstrahlung in a thick conversion target of high element number Z. The photons produce electronpositron pairs and a small fraction of the positrons may be moderated to thermal energies. A review is given of the existing slow positron beam lines using this technique. At accelerator energies of 100 MeV total conversion efficiencies of several slow positrons per 106 primary electrons have been obtained, resulting in average intensities of several 109 slow positrons per second or more than 105 slow positrons in pulses having a…

PhysicsNuclear and High Energy PhysicsHigh energyPhotonBremsstrahlungElectronCondensed Matter PhysicsAtomic and Molecular Physics and OpticsIntensity (physics)Nuclear physicsPositronThermalPhysics::Accelerator PhysicsPhysical and Theoretical ChemistryAtomic physicsOrder of magnitudeHyperfine Interactions
researchProduct

High-power production targets for the Super-FRS using a fast extraction scheme

2003

Abstract The high-power production target of the Super-FRS [H. Geissel et al., these Proceedings] will be irradiated by very intense heavy-ion beams which will be delivered from the future SIS100/200 [An International Accelerator Facility for Beams of Ions and Antiprotons, GSI-Report, 2001] synchrotron facility at the Gesellschaft fur Schwerionenforschung (GSI) Darmstadt. This paper presents calculations of the thermodynamic and the hydrodynamic response of such a target, considering that a uranium ion beam with an energy of 1 GeV/u and an intensity of 10 12 particles will impinge within 50 ns on a solid carbon target with a thickness of 4 g/cm 2 . Due to the high beam intensity the target …

PhysicsNuclear and High Energy PhysicsIon beamCharged particleSynchrotronIonlaw.inventionNuclear physicsAntiprotonlawIrradiationInstrumentationIntensity (heat transfer)Beam (structure)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
researchProduct

High-statistics measurement of the β-delayed α spectrum of 20Na

2013

A measurement of the 20Na β-delayed alpha spectrum with a high-granularity setup has allowed the decay scheme to be revised on several points. Three new transitions of low intensity are found at low α -particle energy. An R-matrix fit of the complete spectrum gives an improved description of the decay and indicates feeding to the broad 2+ α-cluster state close to 9MeV. c Societa Italiana di Fisica / Springer-Verlag 2013

PhysicsNuclear and High Energy PhysicsParticle and Nuclear PhysicsDecay schemeNuclear Fusion010308 nuclear & particles physicsSpectrum (functional analysis)FOS: Physical sciencesAlpha (ethology)01 natural sciencesIntensity (physics)Computational physics20Na0103 physical sciencesNuclear Physics Heavy Ions HadronsBeta (velocity)Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentEnergy (signal processing)
researchProduct

The Collinear Fast Beam laser Spectroscopy (Cfbs) experiment at Triumf

2016

Abstract Laser spectroscopy experiments at radioactive ion beam facilities around the world investigate properties of exotic nuclei for scientific endeavours such as, but not limited to, the investigation of nuclear structure. Advancements in experimental sensitivity and performance are continuously needed in order to extend the reach of nuclei that can be measured. The collinear fast beam laser spectroscopy ( Cfbs ) setup at Triumf , coupled to an out-of-plane radio-frequency quadrupole Paul trap, enables measurements of some of the most fundamental nuclear properties for long-lived ground and isomeric states. The first comprehensive overview of the Cfbs experiment is provided along with d…

PhysicsNuclear and High Energy PhysicsPhotonta114Ion beamcollinear laser spectroscopy010308 nuclear & particles physicsbusiness.industrymulti-dimensional data acquisition system01 natural sciences7. Clean energyAcceleration voltagehigh-frequency intensity modulationOpticsData acquisition0103 physical sciencesQuadrupoletime-resolved fluorescence spectroscopyIon trap010306 general physicsSpectroscopybusinessrapid frequency switchingInstrumentationHyperfine structureNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
researchProduct

High brilliance uranium beams for the GSI FAIR

2017

The 40 years old GSI-UNILAC (Universal Linear Accelerator) as well as the heavy ion synchrotron SIS18 will serve as a high current heavy ion injector for the new FAIR (Facility for Antiproton and Ion Research) synchrotron SIS100. In the context of an advanced machine investigation program in combination with the ongoing UNILAC upgrade program, a new uranium beam intensity record (11.5 emA, ${\mathrm{U}}^{29+}$) at very high beam brilliance was achieved recently in a machine experiment campaign. This is an important step paving the way to fulfill the FAIR heavy ion high intensity beam requirements. Results of high current uranium beam measurements applying a newly developed pulsed hydrogen g…

PhysicsNuclear and High Energy PhysicsPhysics and Astronomy (miscellaneous)010308 nuclear & particles physicschemistry.chemical_elementContext (language use)Surfaces and InterfacesUranium01 natural sciencesSynchrotronlaw.inventionNuclear physicsUpgradechemistrylawUniversal linear accelerator0103 physical sciencesPhysics::Accelerator PhysicsFacility for Antiproton and Ion Researchlcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityNuclear Experiment010306 general physicsIntensity (heat transfer)Beam (structure)Physical Review Accelerators and Beams
researchProduct

Search for forbidden?-decays of the drip line nucleus12Be

1994

Beta-coincidentγ-rays have been measured from implanted pure samples of12Be separated at the LISE3 spectrometer at GANIL. An intensity of 0.040(26) % can be estimated for the branching ratio of the isospin forbidden pure-Fermi transition to the 0+ excited state of12B and of 0.008(6)% of the transition to the 1−1 excited state. Both are taken to represent upper limits. The half-life has been re-measured to be 26.1(2.4) ms.

PhysicsNuclear and High Energy PhysicsSpectrometer010308 nuclear & particles physicsBranching fraction[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences3. Good healthIntensity (physics)Nuclear physicsIsospinExcited state0103 physical sciencesNuclear fusionHaloAtomic physics010306 general physicsLine (formation)Zeitschrift f�r Physik A Hadrons and Nuclei
researchProduct

Strength ofJπ=1+Gamow-Teller and isovector spin monopole transitions in double-β-decay triplets

2014

In this work we study systematically the energetics and intensity distributions of Gamow-Teller (GT${}^{\ifmmode\pm\else\textpm\fi{}}$) and isovector spin monopole (IVSM${}^{\ifmmode\pm\else\textpm\fi{}}$) transitions from the ground states of the pairs ($^{76}\mathrm{Ge}$,$^{76}\mathrm{Se}$), ($^{82}\mathrm{Se}$,$^{82}\mathrm{Kr}$), ($^{100}\mathrm{Mo}$,$^{100}\mathrm{Ru}$), ($^{116}\mathrm{Cd}$,$^{116}\mathrm{Sn}$), ($^{128}\mathrm{Te}$,$^{128}\mathrm{Xe}$), ($^{130}\mathrm{Te}$,$^{130}\mathrm{Xe}$), and ($^{136}\mathrm{Xe}$,$^{136}\mathrm{Ba}$), of double-beta-decay initial and final nuclei, to the ${J}^{\ensuremath{\pi}}={1}^{+}$ excited states of the intermediate odd-odd nuclei $^{76}\…

PhysicsNuclear and High Energy PhysicsValence (chemistry)IsovectorExcited stateGiant resonanceQuasiparticleType (model theory)Atomic physicsSpin (physics)Intensity (heat transfer)Physical Review C
researchProduct