Search results for "decay"

showing 10 items of 2087 documents

Production of refractory elements close to the Z=N line using the ion-guide technique

1998

Production of neutron-deficient isotopes of refractory elements in the A = 80-88 region was studied using the IGISOL technique and the 165 MeV Si-32 + Ni-nat reaction. Radioactive isotopes of Y through Mo could be produced up to the M-T = + 1 line. New information on the decay of the A = 82 and 85 nuclei, including a more detailed decay scheme and more accurate half-life for Y-82, was obtained. (C) 1998 Elsevier Science B.V. All rights reserved.

Nuclear and High Energy PhysicsIsotopes of germaniumAnalytical chemistryONLINE[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesY-81Isotopes of oxygenNuclear physicsIsotopes of protactinium0103 physical sciencesNEUTRON-DEFICIENT ISOTOPES010306 general physicsInstrumentationIsotopes of europiumPhysicsDecay schemeIsotope010308 nuclear & particles physicsRefractory metalsIGISOL TECHNIQUEheavy-ion fusion-evaporation reactionsBeta decayrefractory elementsbeta decayDECAY
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Measurement of the phase between strong and electromagnetic amplitudes of J/ψ decays

2019

Kolcu, Onur Buğra (Arel Author)

Nuclear and High Energy PhysicsJ/Psi decayElectron–positron annihilationBESIII; Electromagnetic amplitude; J/ψ decay; Phase; Strong amplitude; High Energy Physics - Experiment; High Energy Physics - Experiment01 natural sciencesHigh Energy Physics - ExperimentNOSubatomär fysikSubatomic Physics0103 physical sciencesJ/ψ decayStrong amplitudeBorn approximation010306 general physicsPhysicsBESIII Electromagnetic amplitude J/ψ decay Phase Strong amplitudeAnnihilation010308 nuclear & particles physicsBranching fractionBESIIIlcsh:QC1-999BESIII; Electromagnetic amplitude; J/ψ decay; Phase; Strong amplitudeAmplitudeElectromagnetic amplitudePhaseHigh Energy Physics::ExperimentRelative phaseAtomic physicsJ/Psi Decaylcsh:Physics
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$Q$-value of the superallowed $\beta$ decay of 62Ga

2006

Masses of the radioactive isotopes 62Ga, 62Zn and 62Cu have been measured at the JYFLTRAP facility with a relative precision of better than 18 ppb. A Q_EC value of (9181.07 +- 0.54) keV for the superallowed decay of 62Ga is obtained from the measured cyclotron frequency ratios of 62Ga-62Zn, 62Ga-62Ni and 62Zn-62Ni ions. The resulting Ft-value supports the validity of the conserved vector current hypothesis (CVC). The mass excess values measured were (-51986.5 +-1.0) keV for 62Ga, (-61167.9 +- 0.9) keV for 62Zn and (-62787.2 +- 0.9) keV for 62Cu.

Nuclear and High Energy PhysicsMass excessQ valuePenning trapCyclotronFOS: Physical sciences27.50.+e; 23.40.-s; 24.80.+g; 21.10.Dr[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyIonlaw.inventionNuclear physicslawDouble beta decayFt value0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsRadionuclide010308 nuclear & particles physicsBeta decayQ-valueAtomic massAtomic mass
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Lead–gold eutectic: An alternative liquid target material candidate for high power spallation neutron sources

2011

Abstract One of the main technical concerns of Megawatt-class spallation neutron sources is the removal of the heat deposited in the target station. A way to overcome it is to use targets consisting of flowing liquid metals, but the already tested materials – mercury and lead–bismuth eutectic (LBE) – are not unproblematic. We show here that another eutectic alloy containing lead and gold (LGE) could be a suitable alternative. Besides a chemical toxicity lower than mercury, this low melting-point alloy has the advantage of being solid at RT. Moreover, it combines a neutron production similar to mercury and LBE with smaller amounts of alpha-emitting nuclides, relieving safety and environmenta…

Nuclear and High Energy PhysicsMaterials science010308 nuclear & particles physicsMetallurgyAlloyRadiochemistrychemistry.chemical_elementengineering.material7. Clean energy01 natural sciencesMercury (element)Nuclear Energy and Engineeringchemistry0103 physical sciencesengineeringNeutron sourceGeneral Materials ScienceSpallationNeutronNuclideDecay heat010306 general physicsEutectic systemJournal of Nuclear Materials
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Measurement of the ratioB(B+→Xeν)/B(B0→Xeν)

2005

We report measurements of the inclusive electron momentum spectra in decays of charged and neutral B mesons, and of the ratio of semileptonic branching fractions B(B+-> Xe nu) and B(B-0 -> Xe nu). These were performed on a sample of 231x10(6) B (B) over bar events recorded with the BABAR detector at the Upsilon(4S) resonance. Events are selected by fully reconstructing a hadronic decay of one B meson and identifying an electron among the decay products of the recoiling (B) over bar meson. We obtain B(B+-> Xe nu)/B(B-0 -> Xe nu)=1.074 +/- 0.041((stat))+/- 0.026((syst)).

Nuclear and High Energy PhysicsMesonmedia_common.quotation_subjectElectron–positron annihilationHadronElementary particleElectronAsymmetry01 natural sciencesNuclear physicsParticle decayTheoretical physicsTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesB mesonNuclear Experiment010306 general physicsmedia_commonBosonPhysicsBranching fraction010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyCrystallographyHigh Energy Physics::ExperimentLeptonPhysical Review D
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β decay studies of n-rich Cs isotopes with the ISOLDE Decay Station

2017

R. Lica et al. -- 14 pags., 7 figs., tab. -- Open Access funded by Creative Commons Atribution Licence 3.0

Nuclear and High Energy PhysicsNEUTRON-RICHnuclear deformationIsotopes of germaniumβ decayMASS[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesISOLDEBA-148Nuclear physicsLA-1480103 physical sciencesNuclear Physics - ExperimentBAND-STRUCTURESNuclear Experiment010306 general physicsPhysicsDecay schemeNUCLEIIsotope010308 nuclear & particles physicsBEAMSBeta decay3. Good healthexotic nucleiPICOSECOND LIFETIME MEASUREMENTSbeta decayAtomic physicsNuclear deformation ISOLDEExotic nucleiJournal of Physics G: Nuclear and Particle Physics
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Relativistic Energy Density Functional Description of Shape Transition in Superheavy Nuclei

2012

Relativistic energy density functionals (REDF) provide a complete and accurate, global description of nuclear structure phenomena. A modern semi-empirical functional, adjusted to the nuclear matter equation of state and to empirical masses of deformed nuclei, is applied to studies of shapes of superheavy nuclei. The theoretical framework is tested in a comparison of calculated masses, quadrupole deformations, and potential energy barriers to available data on actinide isotopes. Self-consistent mean-field calculations predict a variety of spherical, axial and triaxial shapes of long-lived superheavy nuclei, and their alpha-decay energies and half-lives are compared to data. A microscopic, RE…

Nuclear and High Energy PhysicsNuclear TheoryNuclear TheoryFOS: Physical sciences01 natural sciencesNuclear physicssuperheavy nucleiNuclear Theory (nucl-th)0103 physical sciencesalpha-decayNuclear Energy Density Functional; Superheavy Nuclei; alpha-decay010306 general physicsNuclear ExperimentPhysicsIsotopeta114010308 nuclear & particles physicsEquation of state (cosmology)Relativistic energyNuclear structurenuclear energy density functionalActinideNuclear matterPotential energyNATURAL SCIENCES. Physics.3. Good healthPRIRODNE ZNANOSTI. Fizika.QuadrupoleAtomic physics
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Is Seniority a Partial Dynamic Symmetry in the First $\nu g_{9/2}$ Shell?

2018

The low-lying structures of the midshell νg9/2 Ni isotopes 72Ni and 74Ni have been investigated at the RIBF facility in RIKEN within the EURICA collaboration. Previously unobserved low-lying states were accessed for the first time following β decay of the mother nuclei 72Co and 74Co. As a result, we provide a complete picture in terms of the seniority scheme up to the first (8+) levels for both nuclei. The experimental results are compared to shell-model calculations in order to define to what extent the seniority quantum number is preserved in the first neutron g9/2 shell. We find that the disappearance of the seniority isomerism in the (81+) states can be explained by a lowering of the se…

Nuclear and High Energy PhysicsNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Hadron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences29.30.Kv23.40.-sNuclear physics21.60.Cs0103 physical sciencesNeutronSeniority[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]010306 general physicsNuclear Experiment[ PHYS.NUCL ] Physics [physics]/Nuclear Theory [nucl-th]Spin-½Physics010308 nuclear & particles physics23.20.LvFermionQuantum numberlcsh:QC1-999Atomic physicsNucleonlcsh:PhysicsRadioactive decay
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A Precise Measurement of the Tau Lepton Lifetime

1996

The tau lepton lifetime has been measured using three different methods with the DELPHI detector. Two measurements of one-prong decays are combined, accounting for correlations, giving a result of \tau_\tau = 291.8 \pm 3.3 \mbox{ (stat.)} \pm 2.0 \mbox{(sys.) fs} while the decay length distribution of three-prong decays gives the result \tau_{\tau} = 286.7 \pm 4.9 \mbox{ (stat.)} \pm 3.3 \mbox{ (sys.) fs}. Combining the results presented here with previous DELPHI measurements, we get \tau_{\tau} = 291.4 \pm 3.0 fs and find that the ratio of the coupling constant for tau decay relative to that for muon decay is 0.990 \pm 0.009, compatible with lepton universality.

Nuclear and High Energy PhysicsParticle physicsAlephElectron–positron annihilation01 natural sciencesMeasure (mathematics)Partícules (Física nuclear)tau lepton lifetimeNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsZ-DECAYSDELPHICoupling constantPhysicsMuon010308 nuclear & particles physicsDELPHI; tau lepton lifetime; one-prong; three-prongLARGE ELECTRON POSITRON COLLIDERthree-prongYield (chemistry)PARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIone-prongDecay lengthPARTICLE PHYSICSHigh Energy Physics::ExperimentFísica nuclearVertex detectorParticle Physics - ExperimentLepton
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Analysis of the Intermediate-State Contributions to Neutrinoless Double β− Decays

2016

A comprehensive analysis of the structure of the nuclear matrix elements (NMEs) of neutrinoless double beta-minus (0νβ-β-) decays to the0+ground and first excited states is performed in terms of the contributing multipole states in the intermediate nuclei of0νβ-β-transitions. We concentrate on the transitions mediated by the light (l-NMEs) Majorana neutrinos. As nuclear model we use the proton-neutron quasiparticle random-phase approximation (pnQRPA) with a realistic two-nucleon interaction based on the Bonn one-boson-exchangeGmatrix. In the computations we include the appropriate short-range correlations, nucleon form factors, and higher-order nucleonic weak currents and restore the isospi…

Nuclear and High Energy PhysicsParticle physicsArticle SubjectNuclear Theorydouble beta decaynuclear matrix elements01 natural sciencesneutrinoless double beta decayNuclear physicsMatrix (mathematics)0103 physical sciences010306 general physicsNuclear ExperimentPhysicsta114010308 nuclear & particles physicslcsh:QC1-999MAJORANAExcited stateIsospinQuasiparticleNeutrinoMultipole expansionNucleonlcsh:PhysicsAdvances in High Energy Physics
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