Author(s)
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Pesudo, V (Madrid, Inst. Estructura Materia ; Western Cape U. ; iThemba LABS) ; Borge, M J G (Madrid, Inst. Estructura Materia ; CERN ; Gottingen U.) ; Moro, A M (Seville U.) ; Lay, J A (Padua U. ; INFN, Padua) ; Nácher, E (Madrid, Inst. Estructura Materia) ; Gómez-Camacho, J (Seville U. ; CSIC, Madrid) ; Tengblad, O (Madrid, Inst. Estructura Materia) ; Acosta, L (Mexico U.) ; Alcorta, M (Argonne, PHY) ; Alvarez, M A G (Sao Paulo U.) ; Andreoiu, C (Simon Fraser U.) ; Bender, P C (TRIUMF) ; Braid, R (Colorado School of Mines) ; Cubero, M (Madrid, Inst. Estructura Materia ; Costa Rica U.) ; Di Pietro, A (INFN, LNS) ; Fernández-García, J P (Seville U. ; CSIC, Madrid ; INFN, LNS) ; Figuera, P (INFN, LNS) ; Fisichella, M (INFN, LNS) ; Fulton, B R (York U., England) ; Garnsworthy, A B (TRIUMF) ; Hackman, G (TRIUMF) ; Hager, U (Michigan State U., NSCL) ; Kirsebom, O S (TRIUMF ; Aarhus U.) ; Kuhn, K (Colorado School of Mines) ; Lattuada, M (INFN, LNS ; Catania U.) ; Marquínez-Durán, G (Huelva U.) ; Martel, I (Huelva U.) ; Miller, D (TRIUMF) ; Moukaddam, M (TRIUMF) ; O'Malley, P D (Colorado School of Mines) ; Perea, A (Madrid, Inst. Estructura Materia) ; Rajabali, M M (TRIUMF) ; Sánchez-Benítez, A M (Huelva U.) ; Sarazin, F (Colorado School of Mines) ; Scuderi, V (INFN, LNS) ; Svensson, C E (Guelph U.) ; Unsworth, C (TRIUMF) ; Wang, Z M (Simon Fraser U. ; TRIUMF) |
Abstract
| Angular distributions of the elastic, inelastic, and breakup cross sections of the halo nucleus Be11 on $^{197}Au$ were measured at energies below $(E_{lab}=31.9 MeV)$ and around (39.6 MeV) the Coulomb barrier. These three channels were unambiguously separated for the first time for reactions of $^{11}Be$ on a high-Z target at low energies. The experiment was performed at TRIUMF (Vancouver, Canada). The differential cross sections were compared with three different calculations: semiclassical, inert-core continuum-coupled-channels and continuum-coupled-channels ones with including core deformation. These results show conclusively that the elastic and inelastic differential cross sections can only be accounted for if core-excited admixtures are taken into account. The cross sections for these channels strongly depend on the B(E1) distribution in $^{11}Be$, and the reaction mechanism is sensitive to the entanglement of core and halo degrees of freedom in $^{11}Be$. |