Improved precision on the experimental $E0$ decay branching ratio of the Hoyle state

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  • T. K. Eriksen
    Australian National University, Canberra
  • T. Kibédi
    Australian National University, Canberra
  • M. W. Reed
    Australian National University, Canberra
  • A. E. Stuchbery
    Australian National University, Canberra
  • K. J. Cook
    Australian National University, Canberra
  • A. Akber
    Australian National University, Canberra
  • B. Alshahrani
    Australian National University, Canberra
  • A. A. Avaa
    University of the Witwatersrand
  • K. Banerjee
    Australian National University, Canberra
  • A. C. Berriman
    Australian National University, Canberra
  • L. T. Bezzina
    Australian National University, Canberra
  • L. Bignell
    Australian National University, Canberra
  • J. Buete
    Australian National University, Canberra
  • I. P. Carter
    Australian National University, Canberra
  • B. J. Coombes
    Australian National University, Canberra
  • J. T. H. Dowie
    Australian National University, Canberra
  • M. Dasgupta
    Australian National University, Canberra
  • L. J. Evitts
  • A. B. Garnsworthy
    TRIUMF
  • M. S. M. Gerathy
    Australian National University, Canberra
  • T. J. Gray
    Australian National University, Canberra
  • D. J. Hinde
    Australian National University, Canberra
  • T. H. Hoang
    Osaka University
  • S. S. Hota
    Australian National University, Canberra
  • E. Ideguchi
    Osaka University
  • G. J. Lane
    Australian National University, Canberra
  • B. P. McCormick
    Australian National University, Canberra
  • A. J. Mitchell
    Australian National University, Canberra
  • N. Palalani
    Australian National University, Canberra
  • T. Palazzo
    Australian National University, Canberra
  • M. Ripper
    Australian National University, Canberra
  • J. Smallcombe
    TRIUMF
  • B. M. A. Swinton-Bland
    Australian National University, Canberra
  • T. Tanaka
    Australian National University, Canberra
  • T. G. Tornyi
    Australian National University, Canberra
  • M. O. de Vries
    Australian National University, Canberra
Stellar carbon synthesis occurs exclusively via the 3α process, in which three α particles fuse to
form 12C in the excited Hoyle state, followed by electromagnetic decay to the ground state. The Hoyle state is above the α threshold, and the rate of stellar carbon production depends on the radiative width of this state.
The radiative width cannot be measured directly, and must instead be deduced by combining three separately measured quantities. One of these quantities is the E0 decay branching ratio of the Hoyle state, and the current
10% uncertainty on the radiative width stems mainly from the uncertainty on this ratio. The rate of the 3α process is an important input parameter in astrophysical calculations on stellar evolution, and a high precision is imperative to constrain the possible outcomes of astrophysical models.
Original languageEnglish
Pages (from-to)024320
Number of pages1
JournalPhysical Review C
Volume102
Issue number2
Publication statusPublished - 17 Aug 2020
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