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Giraud, S; Zamora, J C; Zegers, R G T; Bazin, D; Ayyad, Y; Bacca, S; Beceiro-Novo, S; Brown, B A; Carls, A; Chen, J; Cortesi, M; DeNudt, M; Hagen, G; Hultquist, C; Maher, C; Mittig, W; Ndayisabye, F; Noji, S; Novario, S J; Pereira, J; Rahman, Z; Schmitt, J; Serikow, M; Sun, L J; Surbrook, J; Watwood, N; Wheeler, T.
Affiliation
  • Giraud S; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Zamora JC; Joint Institute for Nuclear Astrophysics: Center for the Evolution of the Elements, Michigan State University, East Lansing, Michigan 48824, USA.
  • Zegers RGT; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Bazin D; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Ayyad Y; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Bacca S; Joint Institute for Nuclear Astrophysics: Center for the Evolution of the Elements, Michigan State University, East Lansing, Michigan 48824, USA.
  • Beceiro-Novo S; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Brown BA; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Carls A; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Chen J; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Cortesi M; IGFAE, Universidade de Santiago de Compostela, E-15782 Santiago de Compostela, Spain.
  • DeNudt M; Institut für Kernphysik and PRISMA+ Cluster of Excellence, Johannes Gutenberg-Universität, 55128 Mainz, Germany.
  • Hagen G; Helmholtz-Institut Mainz, Johannes Gutenberg-Universität Mainz, D-55099 Mainz, Germany.
  • Hultquist C; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Maher C; CITENI, Campus Industrial de Ferrol, Universidade da Coruña, Campus de Esteiro, 15403 Ferrol, Spain.
  • Mittig W; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Ndayisabye F; Joint Institute for Nuclear Astrophysics: Center for the Evolution of the Elements, Michigan State University, East Lansing, Michigan 48824, USA.
  • Noji S; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Novario SJ; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Pereira J; Joint Institute for Nuclear Astrophysics: Center for the Evolution of the Elements, Michigan State University, East Lansing, Michigan 48824, USA.
  • Rahman Z; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
  • Schmitt J; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Serikow M; Physics Division, Argonne National Laboratory, Lemont, Illinois 60439, USA.
  • Sun LJ; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Surbrook J; Facility for Rare Isotope Beams, Michigan State University, East Lansing, Michigan 48824, USA.
  • Watwood N; Joint Institute for Nuclear Astrophysics: Center for the Evolution of the Elements, Michigan State University, East Lansing, Michigan 48824, USA.
  • Wheeler T; Department of Physics and Astronomy, Michigan State University, East Lansing, Michigan 48824, USA.
Phys Rev Lett ; 130(23): 232301, 2023 Jun 09.
Article in En | MEDLINE | ID: mdl-37354417
ABSTRACT
For the first time, the (d,^{2}He) reaction was successfully used in inverse kinematics to extract the Gamow-Teller transition strength in the ß^{+} direction from an unstable nucleus. The new technique was made possible by the use of an active-target time-projection chamber and a magnetic spectrometer, and opens a path to addressing a range of scientific challenges, including in astrophysics and neutrino physics. In this Letter, the nucleus studied was ^{14}O, and the Gamow-Teller transition strength to ^{14}N was extracted up to an excitation energy of 22 MeV. The data were compared to shell-model and state-of-the-art coupled-cluster calculations. Shell-model calculations reproduce the measured Gamow-Teller strength distribution up to about 15 MeV reasonably well, after the application of a phenomenological quenching factor. In a significant step forward to better understand this quenching, the coupled-cluster calculation reproduces the full strength distribution well without such quenching, owing to the large model space, the inclusion of strong correlations, and the coupling of the weak interaction to two nucleons through two-body currents.
Subject(s)

Full text: 1 Collection: 01-internacional Database: MEDLINE Main subject: Physics / Cell Nucleus Type of study: Prognostic_studies / Qualitative_research Language: En Journal: Phys Rev Lett Year: 2023 Type: Article Affiliation country: United States

Full text: 1 Collection: 01-internacional Database: MEDLINE Main subject: Physics / Cell Nucleus Type of study: Prognostic_studies / Qualitative_research Language: En Journal: Phys Rev Lett Year: 2023 Type: Article Affiliation country: United States