2017
DOI: 10.1103/physrevlett.118.152502
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Scattering of the Halo Nucleus Be11 on Au197

Abstract: Angular distributions of the elastic, inelastic, and breakup cross sections of the halo nucleus ^{11}Be 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 continu… Show more

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Cited by 56 publications
(48 citation statements)
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“…• , and one extending from (θ 12 The previous work [27] illustrated the results of the model by focusing on breakup occuring at fixed distances prior to and after the distance of closest approach, without explicitly considering the lifetime of the 8 Be state involved. Here we show complete Monte Carlo calculations where the impact parameters, reaction distance, the 8 Be excitation energies and lifetimes, and the initial orientation of the α fragments are all stocastically sampled.…”
Section: Results Formentioning
confidence: 99%
See 1 more Smart Citation
“…• , and one extending from (θ 12 The previous work [27] illustrated the results of the model by focusing on breakup occuring at fixed distances prior to and after the distance of closest approach, without explicitly considering the lifetime of the 8 Be state involved. Here we show complete Monte Carlo calculations where the impact parameters, reaction distance, the 8 Be excitation energies and lifetimes, and the initial orientation of the α fragments are all stocastically sampled.…”
Section: Results Formentioning
confidence: 99%
“…At this conference seen talks experimental measurements of reactions of 7 Be (Mazzocco), 8 B (Kolata [11]), and the halo nucleus 11 Be (Pesudo [12]), in addition to time-dependent Hartree-Fock calculations for exotic calcium isotopes (Vo-Phouc [13]). Innovative technical developments were also presented, such as new methods for extraction of fusion excitation functions with stacked targets, which will soon be utilized in experiments with exotic beams (Di Pietro [14,15]).…”
Section: Introductionmentioning
confidence: 99%
“…Also, the decoupling to the continuum of the single-particle or cluster motion of the valence nucleon(s) with respect to the core has motivated the application of reaction models such as continuum-discretized coupled-channels (CDCC) [6], in which the coupling between the elastic and the breakup channel is explicitly taken into account. The CDCC calculations have been applied to study the elastic scattering of exotic neutron-rich nuclei, such as 6 He, 11 Li, and 11 Be, on several medium to heavy target nuclei and at energies around the Coulomb barrier [7][8][9][10][11][12][13][14][15][16][17]. In some of these works, the 11 Be has been described as 10 Be core and a valence neutron while 6 He has been described as a 4 He core and a paired di-neutron system.…”
Section: Introductionmentioning
confidence: 99%
“…This characteristic favors break-up and, therefore, elastic scattering flux absorption, when interacting with another nucleus. Break-up gives rise to a complex problem of three or more bodies and can be driven by different processes: core excitation, direct excitation of the projectile into continuum states, transfer to bound or unbound states of the target, among others [6][7][8][9][10][11][12][13][14]. Close to or even below the Coulomb barrier, the Coulomb break-up can play an important role.…”
Section: Introductionmentioning
confidence: 99%
“…The 11 Li ( 9 Li+n+n) represents another neutron rich exotic nucleus with Borromean structure, therefore, the three binary sub-systems, 9 Li-n and n-n, are not bound. The 11 Li decays, by beta minus emission, in 11 Be, with a half-life of 8.75 (14) ms [24]. There is no bound excited states.…”
Section: Introductionmentioning
confidence: 99%