Search results for "NUCLEOSYNTHESIS"

showing 10 items of 141 documents

The First Three Seconds: a Review of Possible Expansion Histories of the Early Universe

2020

It is commonly assumed that the energy density of the Universe was dominated by radiation between reheating after inflation and the onset of matter domination 54,000 years later. While the abundance of light elements indicates that the Universe was radiation dominated during Big Bang Nucleosynthesis (BBN), there is scant evidence that the Universe was radiation dominated prior to BBN. It is therefore possible that the cosmological history was more complicated, with deviations from the standard radiation domination during the earliest epochs. Indeed, several interesting proposals regarding various topics such as the generation of dark matter, matter-antimatter asymmetry, gravitational waves,…

High Energy Physics - TheoryCosmology and Nongalactic Astrophysics (astro-ph.CO)reheatingmedia_common.quotation_subjectnucleosynthesis: big bangDark matterFOS: Physical sciencesPrimordial black holeGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesCosmologyGeneral Relativity and Quantum Cosmologydark matterGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesis0103 physical sciencesenergy: density010306 general physicsmedia_commonInflation (cosmology)Physics010308 nuclear & particles physicsGravitational wave[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]gravitational radiationAstronomyUniverseinflation: modelBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc]history[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]black hole: primordialasymmetryAstrophysics - Cosmology and Nongalactic Astrophysics
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Approaching the precursor nuclei of the third r-process peak with RIBs

2013

The rapid neutron nucleosynthesis process involves an enormous amount of very exotic neutron-rich nuclei, which represent a theoretical and experimental challenge. Two of the main decay properties that affect the final abundance distribution the most are half-lives and neutron branching ratios. Using fragmentation of a primary $^{238}$U beam at GSI we were able to measure such properties for several neutron-rich nuclei from $^{208}$Hg to $^{218}$Pb. This contribution provides a short update on the status of the data analysis of this experiment, together with a compilation of the latest results published in this mass region, both experimental and theoretical. The impact of the uncertainties …

HistoryNeutron emissionNuclear TheoryFOS: Physical sciencesNeutronPhysics and Astronomy(all)nucl-ex01 natural sciences530EducationNuclear physicsNucleosynthesis/dk/atira/pure/subjectarea/asjc/31000103 physical sciencesNuclear Physics - Experimentddc:530NeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsNeutrons:Energies::Energia nuclear [Àrees temàtiques de la UPC]010308 nuclear & particles physicsBranching fractionNuclear energyComputer Science ApplicationsUranium-238r-processEnergia nuclears-processNucleosynthesisRadioactive decay
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The study of neutron-rich nuclei production in the region of the closed shell N=126 in the multi-nucleon transfer reaction 136Xe+208Pb

2015

Expérience LNL/PRISMA; International audience; The unexplored area of heavy neutron rich nuclei is extremely important for nuclearastrophysics investigations and, in particular, for the understanding of the r-process ofastrophysical nucleogenesis. For the production of heavy neutron rich nuclei located along theneutron closed shell N=126 (probably the last "waiting point" in the r-process of nucleosynthesis)the low-energy multi-nucleon transfer reaction 136Xe+208Pb at Elab=870MeV was explored.Due to the stabilizing eect of the closed neutron shells in both nuclei, N=82 and N=126, andthe rather favorable proton transfer from lead to xenon, the light fragments formed in this processare well b…

Historynuclear astro-physicsProtonNuclear Theoryspektrometritchemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyEducationNuclear physicsXenonNucleosynthesisneutron-rich nuclei0103 physical sciencesNuclear astrophysicschemical elementsNeutron010306 general physicsNuclear ExperimentOpen shellheavy neutron rich nuclei PRISMA spectrometerPhysicsneutron shellsSpectrometer010308 nuclear & particles physicsbeam linesclosed shellsComputer Science Applicationsneutron beamschemistrytime of flightAtomic physicsNucleon
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Slinky inflation

2005

We present a new approach to quintessential inflation, in which both dark energy and inflation are explained by the evolution of a single scalar field. We start from a simple scalar potential with both oscillatory and exponential behavior. We employ the conventional reheating mechanism of new inflation, in which the scalar decays to light fermions with a decay width that is proportional to the scalar mass. Because our scalar mass is proportional to the Hubble rate, this gives adequate reheating at early times while shutting off at late times to preserve quintessence and satisfy nucleosynthesis constraints. We discuss a simple model which solves the horizon, flatness, and "why now" problems.…

Inflation (cosmology)PhysicsNuclear and High Energy PhysicsCosmic microwave backgroundScalar (mathematics)Astrophysics (astro-ph)FOS: Physical sciencesFísicaScalar potentialAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsTheoretical physicsHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)NucleosynthesisDark energyScalar fieldQuintessence
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Mass measurements towards doubly magic Ni-78 : Hydrodynamics versus nuclear mass contribution in core-collapse supernovae

2022

International audience; We report the first high-precision mass measurements of the neutron-rich nuclei 74,75Ni and the clearly identified ground state of 76Cu, along with a more precise mass-excess value of 78Cu, performed with the double Penning trap JYFLTRAP at the Ion Guide Isotope Separator On-Line (IGISOL) facility. These new results lead to a quantitative estimation of the quenching for the N=50 neutron shell gap. The impact of this shell quenching on core-collapse supernova dynamics is specifically tested using a dedicated statistical equilibrium approach that allows a variation of the mass model independent of the other microphysical inputs. We conclude that the impact of nuclear m…

NUCLEOSYNTHESISIONSCore-collapse supernovaNuclear and High Energy PhysicsScience & TechnologyIMPACTPhysicsPenning trapR-PROCESSneutronitAstronomy & Astrophysics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencesSTATEPhysics Particles & FieldsPhysics NuclearSPECTROMETRYPhysical SciencesISOTOPESNuclear massNuclear Physics - ExperimentydinfysiikkaShell gap
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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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Bounds on very low reheating scenarios after Planck

2015

9 pages.- 9 figures

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Astrophysics::High Energy Astrophysical PhenomenaEarly universeFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic AstrophysicsUpper and lower boundsCosmologysymbols.namesakeGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesisPlanckPhysicsCosmology Big Bang NucleosynthesisOscillationHigh Energy Physics::PhenomenologyFísicaHigh Energy Physics - PhenomenologysymbolsProduction (computer science)High Energy Physics::ExperimentNeutrinoAstrophysics - Cosmology and Nongalactic AstrophysicsPrimordial abundance
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Updated BBN bounds on the cosmological lepton asymmetry for non-zero 13

2011

We discuss the bounds on the cosmological lepton number from Big Bang Nucleosynthesis (BBN), in light of recent evidences for a large value of the neutrino mixing angle theta13. The largest asymmetries for electron and muon or tau neutrinos compatible with 4He and 2H primordial yields are computed versus the neutrino mass hierarchy and mixing angles. The flavour oscillation dynamics is traced till the beginning of BBN and neutrino distributions after decoupling are numerically computed. The latter contains in general, non thermal distortion due to the onset of flavour oscillations driven by solar squared mass difference in the temperature range where neutrino scatterings become inefficient …

Nuclear and High Energy PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)media_common.quotation_subjectAstrophysics::High Energy Astrophysical PhenomenaPhysics of the early UniverseFOS: Physical sciences01 natural sciencesAsymmetryPartícules (Física nuclear)symbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesis0103 physical sciencesPrimordial asymmetriesPlanckNeutrinos010306 general physicsNeutrino oscillationmedia_commonPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDecoupling (cosmology)Lepton numberHigh Energy Physics - PhenomenologysymbolsHigh Energy Physics::ExperimentNeutrinoLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
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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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Search for heavy neutrinos mixing with tau neutrinos

2001

We report on a search for heavy neutrinos ($\nus$) produced in the decay $D_s\to \tau \nus$ at the SPS proton target followed by the decay $\nudecay$ in the NOMAD detector. Both decays are expected to occur if $\nus$ is a component of $\nu_{\tau}$.\ From the analysis of the data collected during the 1996-1998 runs with $4.1\times10^{19}$ protons on target, a single candidate event consistent with background expectations was found. This allows to derive an upper limit on the mixing strength between the heavy neutrino and the tau neutrino in the $\nus$ mass range from 10 to 190 $\rm MeV$. Windows between the SN1987a and Big Bang Nucleosynthesis lower limits and our result are still open for f…

Nuclear and High Energy PhysicsParticle physics[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]ProtonFOS: Physical sciences01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Big Bang nucleosynthesisTau neutrino0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsMixing (physics)PhysicsRange (particle radiation)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFísica3. Good healthneutrino mixing; neutrino decayHigh Energy Physics::ExperimentNeutrinoAnomaly (physics)Event (particle physics)Particle Physics - Experiment
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