2002
DOI: 10.1016/s0375-9474(01)01260-x
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Analytical E1 strength functions of two-neutron halo nuclei: the 6He example

Abstract: An analytical model is developed to study the spectra of electromagnetic dissociation of two-neutron halo nuclei without precise knowledge about initial and final states. Phenomenological three-cluster bound state wave functions, reproducing the most relevant features of these nuclei, are used along with no interaction final states. The 6 He nucleus is considered as a test case, and a good agreement with experimental data concerning the shape of the spectrum and the magnitude of the strength function is found.

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Cited by 13 publications
(9 citation statements)
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“…For that purposes we have applied the cluster three-body hyperspherical harmonic model that gives the most simple and physically transparent description of the two-neutron halo structure. To simulate the absence of a bound 21 C we used a shallow 20 C-neutron potential that does not allow 21 C to bind, and we fixed its strength to the required binding energy of 22 C. These simulations show that, to reach the experimentally suggested lower boundary of the extracted matter radius, the separation energy S 2n of two neutrons in 22 C should be of the order of tens of keV, while to reach the mean value the binding must be much weaker. Within the cluster model the matter extension of the nucleus is directly connected to the distance between the matter and charge c.m.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…For that purposes we have applied the cluster three-body hyperspherical harmonic model that gives the most simple and physically transparent description of the two-neutron halo structure. To simulate the absence of a bound 21 C we used a shallow 20 C-neutron potential that does not allow 21 C to bind, and we fixed its strength to the required binding energy of 22 C. These simulations show that, to reach the experimentally suggested lower boundary of the extracted matter radius, the separation energy S 2n of two neutrons in 22 C should be of the order of tens of keV, while to reach the mean value the binding must be much weaker. Within the cluster model the matter extension of the nucleus is directly connected to the distance between the matter and charge c.m.…”
Section: Discussionmentioning
confidence: 99%
“…Within a cluster three-body ( 20 C + n + n) model the bound-state properties of 22 C are defined by the intercluster potentials. The main problem in selecting binary potentials between the constituents is the absence of experimental information about the neutron-core system, beyond the fact that a bound state of 21 C does not exist. Within the shell-model picture this implies that the 1s 1/2 orbit is unbound.…”
Section: A Bound-state Propertiesmentioning
confidence: 99%
“…Our approach will be general in the sense that both neutron-rich and proton-rich systems can be studied. This model was first presented in [5] while similar approaches also exist for one-neutron [6,7] and two-neutron [8][9][10] halo nuclei. Although advanced numerical investigations are readily performed utilizing present day computer power, an analytical approach might have an advantage when exploring general physics features, and the sensitivity to different model assumptions.…”
Section: Introductionmentioning
confidence: 86%
“…"Loosely bound" implies that the nucleus will exhibit a large degree of clusterization. We will consider the case of two clusters, but will also discuss the three-cluster channel (see also similar approaches for one-neutron [3,4,5] and two-neutron [6,7,8] halo nuclei). After a general description of our model we will exemplify it with an application to 8 B.…”
mentioning
confidence: 99%
“…However, concerning the structure of the 8 B ground state, one should keep in mind that the 7 Be core is in itself a weakly bound system with an excited 1/2 − state at 429 keV. The common treatment of 8 B as a two-body system is therefore highly questionable.…”
mentioning
confidence: 99%