Search results for "r-process"

showing 10 items of 74 documents

r -process nucleosynthesis: connecting rare-isotope beam facilities with the cosmos

2018

This is an exciting time for the study of r-process nucleosynthesis. Recently, a neutron star merger GW170817 was observed in extraordinary detail with gravitational waves and electromagnetic radiation from radio to gamma rays. The very red color of the associated kilonova suggests that neutron star mergers are an important r-process site. Astrophysical simulations of neutron star mergers and core collapse supernovae are making rapid progress. Detection of both, electron neutrinos and antineutrinos from the next galactic supernova will constrain the composition of neutrino-driven winds and provide unique nucleosynthesis information. Finally FRIB and other rare-isotope beam facilities will s…

Nuclear and High Energy PhysicsNuclear Theorymedia_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsKilonova01 natural sciences7. Clean energyNuclear Theory (nucl-th)Nucleosynthesis0103 physical sciencesBinary starddc:530Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentStellar evolutionNuclear ExperimentSolar and Stellar Astrophysics (astro-ph.SR)Astrophysics::Galaxy Astrophysicsmedia_commonPhysics010308 nuclear & particles physicsAstronomyUniverseNeutron starSupernovaAstrophysics - Solar and Stellar Astrophysicsr-processJournal of Physics G: Nuclear and Particle Physics
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Supernova bounds on resonant active-sterile neutrino conversions

1997

We discuss the effects of resonant $\nu_e \to \nu_s$ and $\bar{\nu}_e \to \bar{\nu}_s$ ($\nu_s$ is a sterile neutrino) conversions in the dense medium of a supernova. In particular, we assume the sterile neutrino $\nu_s$ to be in the hot dark matter few eV mass range. The implications of such a scenario for the supernova shock re-heating, the detected $\bar\nu_e$ signal from SN1987A and for the r-process nucleosynthesis hypothesis are analysed in some detail. The resulting constraints on mixing and mass difference for the $\nu_e-\nu_s$ system are derived. There is also an allowed region in the neutrino parameter space for which the r-process nucleosynthesis can be enhanced.

Nuclear and High Energy PhysicsParticle physicsSterile neutrinoAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesParameter spaceAstrophysics01 natural sciences7. Clean energyHigh Energy Physics - Phenomenology (hep-ph)Nucleosynthesis0103 physical sciences010306 general physicsAstrophysics::Galaxy AstrophysicsMixing (physics)Physics010308 nuclear & particles physicsHot dark matterAstrophysics (astro-ph)High Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologySupernovar-processHigh Energy Physics::ExperimentNeutrinoPhysical Review D
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Three beta-decaying states in 128In and 130In resolved for the first time using Penning-trap techniques

2020

Isomeric states in 128In and 130In have been studied with the JYFLTRAP Penning trap at the IGISOL facility. By employing state-of-the-art ion manipulation techniques, three different beta-decaying states in 128In and 130In have been separated and their masses measured. JYFLTRAP was also used to select the ions of interest for identification at a post-trap decay spectroscopy station. A new beta-decaying high-spin isomer feeding the isomer in 128Sn has been discovered in 128In at 1797.6(20) keV. Shell-model calculations employing a CD-Bonn potential re-normalized with the perturbative G-matrix approach suggest this new isomer to be a 16⁺ spin-trap isomer. In 130In, the lowest-lying (10⁻) isom…

Nuclear and High Energy PhysicsPenning trapAstronomy & Astrophysics01 natural sciencesIonPhysics Particles & Fieldsbeta-decay spectroscopyIsomersShell model0103 physical sciencesPhysics::Atomic and Molecular ClustersNuclear Experiment010306 general physicsSpectroscopyCouplingPhysicsScience & TechnologyNUCLEI010308 nuclear & particles physicsPhysicsPRECISION MASS-SPECTROMETRYNuclear shell modelR-PROCESSshell modelpenning trapRAMSEY METHODPenning traplcsh:QC1-999Physics NuclearExcited stateBeta (plasma physics)Physical SciencesSHELL-MODELTRANSITION-PROBABILITIESisomersAtomic physicsBeta-decay spectroscopylcsh:PhysicsIon cyclotron resonancePhysics Letters B
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Beta-decay half-lives of very neutron-rich nuclei and their consequences for the astrophysical r-process

2005

Half-lives for Gamow-Teller β-decay of very neutron-rich nuclei have been calculated using the RPA shell-model code of Krumlinde and Muller. For the examples of the isotope sequences of 27Co and 37Rb, and of nuclei around 132Sn it is demonstrated that close agreement between experiment and theory can be obtained, provided an appropriate choice of model parameters is made for each mass region. On the basis of this agreement, T1/2 predictions for isotopes up to the r-process path are made and compared to earlier model calculations. Possible implications of the results on the site and the cycle time of the r-process are discussed.

Nuclear physicsNuclear reactionPhysicsIsotopeBeta particleNuclear astrophysicsr-processNeutronNuclear drip lineRadioactive decay
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About the Reliability of Extrapolation of Nuclear Structure Data for r-process Calculations

2002

Gross decay properties are the nuclear part of the input for calculations of elemental abundances. They depend, sometimes very sensitively, on details of nuclear structure. Models for predictions of nuclear masses and shapes have to be used for isotopes very far from stability. The reliability of extrapolations far from experimentally reachable nuclei is, however, not always granted due to singularities in the nuclear landscape. We review data on the region of the neutron-rich isotopes near A = 100, which is a region of especially dramatic changes.

Nuclear physicsPhysicsIsotopeNeutron numberNuclear TheoryNuclear structureExtrapolationr-processGravitational singularityNuclear ExperimentStability (probability)Reliability (statistics)
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Nuclear Physics Constraints to Bring the Astrophysical R-Process to the “Waiting Point”

1988

Rapid neutron-capture (r-process) nucleosynthesis of heavy elements generally involves the participation of large numbers of stable to highly unstable nuclear species. Most of these properties are experimentally unknown and have to be predicted from nuclear models. So far, the uncertainties of such predictions have not allowed putting substantial constraints on astrophysical scenarios. For the classical r-process it is shown that the s-decay properties of only a few key-nuclei, i.e. the recently measured “waiting-point” nuclei 130Cd82 and 80Zn50 together with new shell-model predictions for their N ≈ 82 and 50 neighbours, may be sufficient to explain the observed r-abundances in the A ≈ 130…

Nuclear physicsPhysicsNeutron captureNucleosynthesisAbundance (ecology)r-processPoint (geometry)AstrophysicsNeutron density
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Nuclear structure theory for the astrophysical rp-process and r-process

2003

Abstract The astrophysical processes of rapid-proton capture and rapid-neutron capture require the knowledge of many nuclear properties which are not known from experiment. I will describe two examples of how theoretical models are used to provide this input. The first of these uses the Hartree-Fock method for displacement energies to obtain the masses of proton-rich nuclei needed for the rp-process. The second uses a model for configuration mixing near 132 Sn to provide Q values and beta-decay lifetimes for the r-process.

Nuclear physicsPhysicsNuclear and High Energy PhysicsAstrophysical ProcessesMixing (mathematics)Nuclear TheoryNuclear structureTheoretical modelsr-processrp-processNuclear ExperimentDisplacement (vector)Nuclear Physics A
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Neutron-rich isotopes around the r-process ?waiting-point? nuclei 29 79 Cu50 and 30 80 Zn50

1991

Beta-decay half-lives (T1/2) and delayed-neutron emission probabilities (Pn) of very neutron-rich Cu to As nuclei have been measured, among them the new isotopes77Cu48,79Cu50,81Zn51 and84Ga53. With the T1/2 and Pn-values of now four N ∼-50 ”waiting-point” nuclei known, our hypothesis that the r-process has attained a local β-flow equilibrium araound A∼-80 is further strengthened.

Nuclear physicsPhysicsNuclear and High Energy PhysicsIsotoper-processNuclear fusionPoint (geometry)NeutronAtomic physicsZeitschrift f�r Physik A Hadrons and Nuclei
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Nuclear-structure input to r-process calculations

1998

Abstract By comparing results from r-process parameter studies within the classical waiting-point approximation with the observed solar-system r-abundance distribution N r ,⊙ , in-formation on nuclear-structure phenomena on neutron-rich isotopes far off the stability line can be obtained. Such information is — to a large extent — experimentally not accessible. Investigations in the early 1990's, making use of QRPA β-decay properties and nuclear masses from the macroscopic-microscopic FRDM and ETFSI-1 models, showed r-abundance deficiencies around A ⋍115 and 180 , indicating overly strong N=82 and 126 shell strengths far from stability. Recent experiments in the A ⋍110–130 region as well as …

Nuclear physicsPhysicsNuclear and High Energy PhysicsStarsFormalism (philosophy of mathematics)IsotopeNuclear TheoryNuclear structurer-processNeutronHaloAnsatzNuclear Physics A
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β-decay studies of r-process nuclei at NSCL

2008

Abstract Observed neutron-capture elemental abundances in metal-poor stars, along with ongoing analysis of the extremely metal-poor Eu-enriched sub-class provide new guidance for astrophysical models aimed at finding the r-process sites. The present paper emphasizes the importance of nuclear physics parameters entering in these models, particularly β -decay properties of neutron-rich nuclei. In this context, several r-process motivated β -decay experiments performed at the National Superconducting Cyclotron Laboratory (NSCL) are presented, including a summary of results and impact on model calculations.

Nuclear physicsPhysicsNuclear and High Energy PhysicsStarsSuperconducting cyclotronDouble beta decayr-processContext (language use)Nuclear ExperimentBeta decayNuclear Physics A
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