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Ong, W-J; Brown, E F; Browne, J; Ahn, S; Childers, K; Crider, B P; Dombos, A C; Gupta, S S; Hitt, G W; Langer, C; Lewis, R; Liddick, S N; Lyons, S; Meisel, Z; Möller, P; Montes, F; Naqvi, F; Pereira, J; Prokop, C; Richman, D; Schatz, H; Schmidt, K; Spyrou, A.
Afiliação
  • Ong WJ; Nuclear and Chemical Sciences Division, Lawrence Livermore National Laboratory, Livermore, California 94550, USA.
  • Brown EF; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Browne J; National Superconducting Cyclotron Laboratory, East Lansing, Michigan 48824, USA.
  • Ahn S; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Childers K; National Superconducting Cyclotron Laboratory, East Lansing, Michigan 48824, USA.
  • Crider BP; Joint Institute for Nuclear Astrophysics-Center for the Evolution of the Elements, Michigan State University, East Lansing, Michigan 48824, USA.
  • Dombos AC; Department of Computational Mathematics, Science, and Engineering, Michigan State University, East Lansing, Michigan 48824, USA.
  • Gupta SS; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Hitt GW; National Superconducting Cyclotron Laboratory, East Lansing, Michigan 48824, USA.
  • Langer C; Joint Institute for Nuclear Astrophysics-Center for the Evolution of the Elements, Michigan State University, East Lansing, Michigan 48824, USA.
  • Lewis R; Cylotron Institute, Texas A&M University, College Station, Texas 77843, USA.
  • Liddick SN; National Superconducting Cyclotron Laboratory, East Lansing, Michigan 48824, USA.
  • Lyons S; Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA.
  • Meisel Z; Department of Physics and Astronomy, Mississippi State University, Mississippi State, Mississippi 39762, USA.
  • Möller P; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Montes F; National Superconducting Cyclotron Laboratory, East Lansing, Michigan 48824, USA.
  • Naqvi F; Joint Institute for Nuclear Astrophysics-Center for the Evolution of the Elements, Michigan State University, East Lansing, Michigan 48824, USA.
  • Pereira J; Indian Institute of Technology Ropar, Nangal Road, Rupnagar (Ropar), Punjab 140 001, India.
  • Prokop C; Department of Physics and Engineering Science, Coastal Carolina University, Conway, South Carolina 29528, USA.
  • Richman D; Institute for Applied Physics, Goethe-University Frankfurt a. M., Frankfurt am Main 60438, Germany.
  • Schatz H; National Superconducting Cyclotron Laboratory, East Lansing, Michigan 48824, USA.
  • Schmidt K; Department of Chemistry, Michigan State University, East Lansing, Michigan 48824, USA.
  • Spyrou A; National Superconducting Cyclotron Laboratory, East Lansing, Michigan 48824, USA.
Phys Rev Lett ; 125(26): 262701, 2020 Dec 31.
Article em En | MEDLINE | ID: mdl-33449748
ABSTRACT
The interpretation of observations of cooling neutron star crusts in quasipersistent x-ray transients is affected by predictions of the strength of neutrino cooling via crust Urca processes. The strength of crust Urca neutrino cooling depends sensitively on the electron-capture and ß-decay ground-state-to-ground-state transition strengths of neutron-rich rare isotopes. Nuclei with a mass number of A=61 are predicted to be among the most abundant in accreted crusts, and the last remaining experimentally undetermined ground-state-to-ground-state transition strength was the ß decay of ^{61}V. This Letter reports the first experimental determination of this transition strength, a ground-state branching of 8.1_{-3.1}^{+4.0}%, corresponding to a log ft value of 5.5_{-0.2}^{+0.2}. This result was achieved through the measurement of the ß-delayed γ rays using the total absorption spectrometer SuN and the measurement of the ß-delayed neutron branch using the neutron long counter system NERO at the National Superconducting Cyclotron Laboratory at Michigan State University. This method helps to mitigate the impact of the pandemonium effect in extremely neutron-rich nuclei on experimental results. The result implies that A=61 nuclei do not provide the strongest cooling in accreted neutron star crusts as expected by some predictions, but that their cooling is still larger compared to most other mass numbers. Only nuclei with mass numbers 31, 33, and 55 are predicted to be cooling more strongly. However, the theoretical predictions for the transition strengths of these nuclei are not consistently accurate enough to draw conclusions on crust cooling. With the experimental approach developed in this work, all relevant transitions are within reach to be studied in the future.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2020 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2020 Tipo de documento: Article