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. PucknellK. Riisager, S. Rinta-Antila, O. Tengblad, Y. Wang, K. Wilhelmsen, J. Äystö

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    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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