Labiche M, Orr NA, Marqués FM, Angélique JC, Axelsson L, Benoit B, Bergmann UC, Borge MJ, Catford WN, Chappell SP, Clarke NM, Costa G, Curtis N, D'Arrigo A, de Góes Brennand E, Dorvaux O, Fazio G, Freer M, Fulton BR, Giardina G, Grévy S, Guillemaud-Mueller D, Hanappe F, Heusch B, Jones KL, Jonson B, Le Brun C, Leenhardt S, Lewitowicz M, Lopez MJ, Markenroth K, Mueller AC, Nilsson T, Ninane A, Nyman G, de Oliveira F, Piqueras I, Riisager K, Saint Laurent MG, Sarazin F, Singer SM, Sorlin O, Stuttgé L. Halo structure of (14)Be.
Phys Rev Lett 2001;
86:600-603. [PMID:
11177891 DOI:
10.1103/physrevlett.86.600]
[Citation(s) in RCA: 3] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/06/2000] [Indexed: 05/23/2023]
Abstract
The two-neutron halo nucleus (14)Be has been investigated in a kinematically complete measurement of the fragments ((12)Be and neutrons) produced in dissociation at 35 MeV/nucleon on C and Pb targets. Two-neutron removal cross sections, neutron angular distributions, and invariant mass spectra were measured, and the contributions from electromagnetic dissociation (EMD) were deduced. Comparison with three-body model calculations suggests that the halo wave function contains a large nu(2s(1/2))(2) admixture. The EMD invariant mass spectrum exhibited enhanced strength near threshold consistent with a nonresonant soft-dipole excitation.
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