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  • The unbound isotopes He-9,H...
    Johansson, Håkan T; Aksyutina, Yuliya; Aumann, T.; Boretzky, K.; Borge, M. J. G.; Chatillon, A.; Chulkov, L. V.; Cortina-Gil, D.; Pramanik, U. D.; Emling, H.; Forssen, Christian; Fynbo, H. O. U.; Geissel, H.; Ickert, G.; Jonson, Björn; Kulessa, R.; Langer, C.; Lantz, Mattias; LeBleis, T.; Mahata, K.; Meister, Mikael; Munzenberg, G.; Nilsson, Thomas; Nyman, Göran Hugo; Palit, R.; Paschalis, S.; Prokopowicz, W.; Reifarth, R.; Richter, A.; Riisager, K.; Schrieder, G.; Simon, H.; Summerer, K.; Tengblad, O.; Weick, H.; Zhukov, Mikhail

    Nuclear physics. A, 2010, Letnik: 842, Številka: 1-4
    Journal Article

    The unbound nuclei He-9 and He-10 have been produced in proton-knockout reactions from a 280 MeV/u Li-11 beam impinging on a liquid hydrogen target at the ALADIN-LAND setup at GSI. Information on their nuclear structure has been obtained from the relative-energy spectra, He-8 + n and He-8 + 2n, employing reaction models incorporating the structure of Li-11. The (8H)e + n relative-energy spectrum is dominated by a strong peak-like structure at low energy, which may be interpreted within the effective-range approximation as the result of an s-wave interaction with a neutron scattering length of -3.17(66) fm. This spectrum also shows evidence for resonance states at 1.33(8) MeV and at 2.4 MeV above the He-8 + n threshold. It is argued that the s-state might not be the He-9 ground state. For He-8 + n + n, the analysis of the relative-energy spectrum gives two alternative possibilities for an interpretation: either a narrow resonance at 1.42(10) MeV (Gamma = 1.11(76) MeV) superimposed on a correlated background, or two overlapping resonances, a ground state at 1.54(11) MeV (Gamma = 1.91(41) MeV) together with an excited state at 3.99(26) MeV (Gamma = 1.64(89) MeV). The two possible interpretations are discussed. (C) 2010 Elsevier B.V. All rights reserved.