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Breakup channels for C12 triple-α continuum states

  • C. Aa Diget
  • , F. C. Barker
  • , M. J.G. Borge
  • , R. Boutami
  • , P. Dendooven
  • , T. Eronen
  • , S. P. Fox
  • , B. R. Fulton
  • , H. O.U. Fynbo
  • , J. Huikari
  • , S. Hyldegaard
  • , H. B. Jeppesen
  • , A. Jokinen
  • , B. Jonson
  • , A. Kankainen
  • , I. Moore
  • , A. Nieminen
  • , G. Nyman
  • , H. Penttilä
  • , V. F.E. Pucknell
  • K. Riisager, S. Rinta-Antila, O. Tengblad, Y. Wang, K. Wilhelmsen, J. Äystö

    Research output: Contribution to journal › Article › peer-review

    21 Citations (Scopus)

    Abstract

    The triple-α-particle breakup of states in the triple-α continuum of C12 has been investigated by way of coincident detection of all three α particles of the breakup. The states have been fed in the β decay of N12 and B12, and the α particles measured using a setup that covers all of the triple-α phase space. Contributions from the breakup through the Be8(0+) ground state as well as other channels-interpreted as breakup through excited energies in Be8-have been identified. Spins and parities of C12 triple-α continuum states are deduced from the measured phase-space distributions for breakup through Be8 above the ground state by comparison to a fully symmetrized sequential R-matrix description of the breakup. At around 10 MeV in C12, the breakup is found to be dominated by 0+ strength breaking up through the ghost of the Be8(0+) ground state with L=0 angular momentum between the first emitted α particle and the intermediate Be8 nucleus. For C12 energies above the 12.7 MeV 1+ state, however, L=2 breakup of a C12 2+ state through the Be8(2+) excited state dominates. Furthermore, the possibility of a 2+ excited state in the 9-12 MeV region of C12 is investigated.

    Original languageEnglish
    Article number034316
    JournalPhysical Review C - Nuclear Physics
    Volume80
    Issue number3
    DOIs
    Publication statusPublished - 22 Sept 2009

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