Search results for "rp-process"

showing 10 items of 25 documents

Isomeric state of $^{80}$Y and its role in the astrophysical rp-process

2001

5 pages, 7 figures.-- PACS nrs: 21.10.Tg; 23.20.Nx; 27.50.+e.

59 ≤ A ≤ 89 [[PACS] Properties of specific nuclei listed by mass ranges]PhysicsNuclear and High Energy Physics[PACS] Properties of specific nuclei listed by mass ranges: 59 ≤ A ≤ 89Proton[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]010308 nuclear & particles physicsHadronElectron[PACS] Internal conversion and extranuclear effects (including Auger electrons and internal bremsstrahlung)rp-processNuclear isomer[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyNuclear physicsExcited state0103 physical sciences[PACS] Lifetimes widthsAtomic physics010306 general physicsInternal conversion coefficientExcitation
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Experimental study of the 15O(2p, γ)17Ne cross section by Coulomb Dissociation for the rp process

2016

6th Nuclear Physics in Astrophysics Conference (NPA), Lisbon, Portugal, 19 May 2013 - 24 May 2013; Journal of physics / Conference Series 665, 012046 (2016). doi:10.1088/1742-6596/665/1/012046

HistoryChemistryNuclear structurechemistry.chemical_elementrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530Dissociation (chemistry)Computer Science ApplicationsEducationIonSubatomär fysikFragmentation (mass spectrometry)Subatomic PhysicsCoulombNuclear Physics - ExperimentBerylliumAtomic physicsNuclear Experiment[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Excitation
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Mass Measurements with the CSS2 and CIME cyclotrons at GANIL

2005

Commune avec ACEN; This paper presents two original direct mass-measurement techniques developed at GANIL using the CSS2 and CIME cyclotrons as high-resolution mass spectrometers. The mass measurement with the CSS2 cyclotron is based on a time-of-flight method along the spiral trajectory of the ions inside the cyclotron. The atomic mass excesses of 68Se and 80Y recently measured with this technique are -53.958(246) MeV and -60.971(180) MeV, respectively. The new mass-measurement technique with the CIME cyclotron is based on the sweep of the acceleration radio-frequency of the cyclotron. Tests with stable beams have been performed in order to study the accuracy of this new mass-measurement m…

Mass numberChemistryCyclotron020206 networking & telecommunicationsParticle accelerator02 engineering and technologyrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryAtomic masslaw.inventionIonNuclear physicsAccelerationlaw29.20.Hm 29.30.-h 21.10.Dr 27.50.+e0202 electrical engineering electronic engineering information engineering020201 artificial intelligence & image processing
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Isomeric state of 80Y and its role in the rp-process

2003

The HIGISOL facility has been used to investigate carefully the isomeric transition 228.5 keV in 80Y. We have measured the electron internal conversion coefficient for this transition αK = 0.50 ± 0.07 which gives the value for half-life of “bare” isomeric state T 1/2 = 6.8 ± 0.5 s. The isomeric state should play an important role in the rp-process calculations.

Materials scienceThermodynamicsElectronState (functional analysis)rp-processNuclear isomerInternal conversion coefficientValue (mathematics)
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Proton decay of 108I and its significance for the termination of the astrophysical rp-process

2019

Abstract Employing the Argonne Fragment Mass Analyzer and the implantation-decay-decay correlation technique, a weak 0.50(21)% proton decay branch was identified in 108I for the first time. The 108I proton-decay width is consistent with a hindered l = 2 emission, suggesting a d 5 2 origin. Using the extracted 108I proton-decay Q value of 597(13) keV, and the Q α values of the 108I and 107Te isotopes, a proton-decay Q value of 510(20) keV for 104Sb was deduced. Similarly to the 112,113Cs proton-emitter pair, the Q p ( I 108 ) value is lower than that for the less-exotic neighbor 109I, possibly due to enhanced proton-neutron interactions in N ≈ Z nuclei. In contrast, the present Q p ( Sb 104 …

Nuclear and High Energy Physicsalpha decayProton decayQ valueastrofysiikkaNuclear Theory104Sb01 natural sciencesastrophysical rp process108I0103 physical sciencesMass analyzer107Te010306 general physicsNuclear ExperimentPhysicsIsotopeta114010308 nuclear & particles physicsInteraction energyrp-processlcsh:QC1-999proton decayHigh Energy Physics::ExperimentAtomic physicsydinfysiikkalcsh:PhysicsPhysics Letters B
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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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New experimental efforts along the rp-process path

2007

The level structure just above the proton threshold of the nucleus 30S has been studied using the neutron removal process on fast radioactive beams at the National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University. In this work we provide a description of the experimental setup. The present status of the analysis is also discussed.

Nuclear physicsPhysicsNuclear and High Energy PhysicsSuperconducting cyclotronProtonNuclear TheoryPath (graph theory)Physics::Accelerator PhysicsLevel structureNeutronrp-processNuclear ExperimentJournal of Physics G: Nuclear and Particle Physics
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Nucleosynthesis of proton-rich nuclei. Experimental results on the rp-process

2009

Experience NSCL; International audience; We report in this study the nuclear properties of proton-rich isotopes located along the rp-process path. The experiments have recently been performed at the National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University. The level properties above the proton separation energy of the nuclei 30S, 36K and 37Ca were measured with precision of < 10 keV. This will allow a reduction in the determination of the astrophysical (p, ) reaction rate under rp-process conditions.

Nuclear reactionPhysicsHistoryProton010308 nuclear & particles physics[SDU.ASTR.SR]Sciences of the Universe [physics]/Astrophysics [astro-ph]/Solar and Stellar Astrophysics [astro-ph.SR]Nuclear TheoryCyclotronrp-process[PHYS.ASTR.SR]Physics [physics]/Astrophysics [astro-ph]/Solar and Stellar Astrophysics [astro-ph.SR]7. Clean energy01 natural sciencesComputer Science ApplicationsEducationlaw.inventionNuclear physicsIsotopes of potassiumlawNucleosynthesis0103 physical sciencesr-processAtomic physics010306 general physicsNuclear ExperimentRadioactive decay
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Mass Measurements for the rp Process

2017

Penning-trap mass spectrometrynovaePhysicsatomic massesChromatographyta114010308 nuclear & particles physicsrp process0103 physical sciencesrp-process010306 general physics01 natural sciencesProceedings of the 14th International Symposium on Nuclei in the Cosmos (NIC2016)
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Low-lying level structure of Cu56 and its implications for the rp process

2017

The low-lying energy levels of proton-rich Cu56 have been extracted using in-beam γ-ray spectroscopy with the state-of-the-art γ-ray tracking array GRETINA in conjunction with the S800 spectrograph at the National Superconducting Cyclotron Laboratory at Michigan State University. Excited states in Cu56 serve as resonances in the Ni55(p,γ)Cu56 reaction, which is a part of the rp process in type-I x-ray bursts. To resolve existing ambiguities in the reaction Q value, a more localized isobaric multiplet mass equation (IMME) fit is used, resulting in Q=639±82 keV. We derive the first experimentally constrained thermonuclear reaction rate for Ni55(p,γ)Cu56. We find that, with this new rate, the …

Physics010308 nuclear & particles physicsQ valuerp-process01 natural sciencesNuclear physicsMass formulaExcited state0103 physical sciencesLevel structureIsobaric processAtomic physics010306 general physicsSpectroscopyMultipletPhysical Review C
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