24.5 A MeV 6He+ p elastic and inelastic scattering

The structure of 6He is explored with proton elastic and inelastic scattering to the first 2 + excited state ( Q=−1.8 MeV) of 6He in the inverse kinematics using a 24.5 A MeV 6He beam. The distorted wave approximation (DWA) with an optical potential obtained by folding an effective nucleon–nucleon (...

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Published inPhysics letters. B Vol. 542; no. 1; pp. 35 - 42
Main Authors Stepantsov, S.V, Bogdanov, D.D, Fomichev, A.S, Rodin, A.M, Sidorchuk, S.I, Slepnev, R.S, Ter-Akopian, G.M, Wolski, R, Chelnokov, M.L, Gorshkov, V.A, Oganessian, Yu.Ts, Alamanos, N, Auger, F, Lapoux, V, Lobo, G, Amos, K, Deb, P.K, Karataglidis, S, Golovkov, M.S, Korsheninnikov, A.A, Tanihata, I, Kuzmin, E.A, Nikolskii, E.Yu, Kavalov, R.L
Format Journal Article
LanguageEnglish
Published Elsevier B.V 01.08.2002
Subjects
Halo nuclei
Inelastic proton scattering
Microscopic calculations
Microscopic calculations
24.10.Eq
23.20.Js
Halo nuclei
Inelastic proton scattering
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Summary:The structure of 6He is explored with proton elastic and inelastic scattering to the first 2 + excited state ( Q=−1.8 MeV) of 6He in the inverse kinematics using a 24.5 A MeV 6He beam. The distorted wave approximation (DWA) with an optical potential obtained by folding an effective nucleon–nucleon (NN) g-matrix with the 6He density matrix elements as given by a large basis shell model is used to analyse the data. The comparison of predictions with the data confirms the view that 6He has an extended (halo) neutron matter distribution.
ISSN:0370-2693
1873-2445
DOI:10.1016/S0370-2693(02)02308-0