Authors

Affiliations

  1. Department of Physics and Astronomy, Springfield University, Springfield, USA.
  2. Institute of Nuclear Structure, Springfield Research Center, Springfield, USA.
  3. Global Research Facility, Springfield, USA.
  4. National Institute for Physics and Nuclear Studies, Springfield, USA.
  5. Department of Physics, University of Central City, Central City, USA.
  6. Advanced Research Center, Springfield, USA.
  7. Department of Physics, North City University, North City, USA.
  8. Department of Physics, South City University, South City, USA.
  9. Institute of Nuclear and Radiation Physics, Springfield University, Springfield, USA.
  10. Nuclear Physics Group, University of Western Springfield, Western Springfield, USA.
  11. Department of Physics, East City University, East City, USA.
  12. Institute of Physics, University of North Springfield, North Springfield, USA.
  13. Laboratory of Nuclear Studies, University of Greater Springfield, Greater Springfield, USA.
  14. National Laboratory for Advanced Physics, Springfield, USA.
  15. GANIL, CEA/DSM-CNRS/IN2P3, Caen, France.
  16. Institute of Nuclear Physics, Technical University of Springfield, Springfield, USA.
  17. GSI Helmholtzzentrum für Schwerionenforschung, Springfield, USA.
  18. Institute of Physics, University of South Springfield, South Springfield, USA.

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PMID: 30339438
DOI: 10.1103/PhysRevLett.121.142701

Abstract

The ^{12}C(α,γ)^{16}O reaction is pivotal in astrophysics; however, laboratory data offer limited constraints on its cross section at energies significant for astrophysical applications. A critical factor in determining this cross section is the reduced α width, γ_{11}, of the bound 1^{-} state in ^{16}O. The value of γ_{11} is obtained through sub-Coulomb α-transfer reactions or β-delayed α decay.

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To Summarize

This study presents the first accurate normalization of the β-delayed α decay of ^{16}N, shedding light on the astrophysical reaction rate of ^{12}C(α,γ)^{16}O. A better understanding of this reaction is crucial for astrophysical models and can lead to improved predictions in stellar nucleosynthesis processes.