1. Structure of 13Be probed via secondary-beam reactions.
- Author
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Randisi, G., Leprince, A., Falou, H. Al, Orr, N. A., Marqués, F. M., Achouri, N. L., Angélique, J. -C., Ashwood, N., Bastin, B., Bloxham, T., Brown, B. A., Catford, W. N., Curtis, N., Delaunay, F., Freer, M., de Goes Brennand, E., Haigh, P., Hanappe, F., Harlin, C., and Laurent, B.
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NUCLEAR size (Physics) , *FRAGMENTATION reactions , *PROTONS , *SPECTRUM analysis , *CYCLOTRONS - Abstract
The low-lying level structure of the unbound neutron-rich nucleus 13Be has been investigated via breakup on a carbon target of secondary beams of 14,15B at 35 MeV/nucleon. The coincident detection of the beam velocity 12Be fragments and neutrons permitted the invariant mass of the 12Be+n and 12Be+n+n systems to be reconstructed. In the case of the breakup of 15B, a very narrow structure at threshold was observed in the 12Be+n channel. Analysis of the 12Be+n+n events demonstrated that this resulted from the sequential decay of the unbound 14Be(2+) state rather than a strongly interacting s-wave virtual state in 13Be, as had been surmised in stable beam fragmentation studies. Single-proton removal from 14B was found to populate a broad low-lying structure some 0.7 MeV above the neutron-decay threshold, in addition to a less prominent feature at around 2.4 MeV. Based on the selectivity of the reaction and a comparison with (0-3)... shell-model calculations, the low-lying structure is concluded to arise from closely spaced Jp=1/2+ and 5/2+ resonances (Er=0.40±0.03 and 0.85-0.11+0.15 MeV), while the broad higher-lying feature is a second 5/2+ level (Er=2.35±0.14 MeV). Taken in conjunction with earlier studies, the results suggest that the lowest 1/2+ and 1/2- levels lie relatively close together below 1 MeV. [ABSTRACT FROM AUTHOR]
- Published
- 2014
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