0000000000393844

AUTHOR

Yukie Maeda

showing 3 related works from this author

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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Nonquenched Isoscalar Spin-M1Excitations insd-Shell Nuclei

2015

Differential cross sections of isoscalar and isovector spin-M1 (0(+)→1(+)) transitions are measured using high-energy-resolution proton inelastic scattering at E(p)=295  MeV on (24)Mg, (28)Si, (32)S, and (36)Ar at 0°-14°. The squared spin-M1 nuclear transition matrix elements are deduced from the measured differential cross sections by applying empirically determined unit cross sections based on the assumption of isospin symmetry. The ratios of the squared nuclear matrix elements accumulated up to E(x)=16  MeV compared to a shell-model prediction are 1.01(9) for isoscalar and 0.61(6) for isovector spin-M1 transitions, respectively. Thus, no quenching is observed for isoscalar spin-M1 transi…

PhysicsMatrix (mathematics)IsovectorProtonIsospinIsoscalarNuclear TheoryStochastic matrixGeneral Physics and AstronomyInelastic scatteringAtomic physicsNuclear ExperimentSpin (physics)Physical Review Letters
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Determining therp-Process Flow throughNi56: Resonances inCu57(p,γ)Zn58Identified with GRETINA

2014

An approach is presented to experimentally constrain previously unreachable (p, γ) reaction rates on nuclei far from stability in the astrophysical rp process. Energies of all critical resonances in the (57)Cu(p,γ)(58)Zn reaction are deduced by populating states in (58)Zn with a (d, n) reaction in inverse kinematics at 75 MeV/u, and detecting γ-ray-recoil coincidences with the state-of-the-art γ-ray tracking array GRETINA and the S800 spectrograph at the National Superconducting Cyclotron Laboratory. The results reduce the uncertainty in the (57)Cu(p,γ) reaction rate by several orders of magnitude. The effective lifetime of (56)Ni, an important waiting point in the rp process in x-ray burst…

PhysicsReaction rateChemical substanceSuperconducting cyclotronOrders of magnitude (time)Radiative captureFlow (psychology)Analytical chemistryGeneral Physics and Astronomyrp-processNuclear ExperimentPhysical Review Letters
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