2014
DOI: 10.1103/physrevc.90.034303
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Role of diproton correlation in two-proton-emission decay of theBe6nucleus

Abstract: We discuss a role of diproton correlation in two-proton emission from the ground state of a proton-rich nucleus, 6 Be. Assuming the three-body structure of α + p + p configuration, we develop a time-dependent approach, in which the two-proton emission is described as a time-evolution of a three-body metastable state. With this method, the dynamics of the two-proton emission can be intuitively discussed by monitoring the time-dependence of the two-particle density distribution. With a model Hamiltonian which we… Show more

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Cited by 28 publications
(65 citation statements)
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References 72 publications
(153 reference statements)
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“…It is worthwhile to mention that, if one can neglect PCE, 2p-resonance state locates at Q 2p = h 1 + h 2 = 2ǫ r , where ǫ r is the α − p resonance energy. In this case, where 2p-wave function keeps the pure (p 3/2 ) 2 configuration, it was confirmed that the decay process is well described as a sequential 2p emission [33].…”
Section: Three-body Modelsupporting
confidence: 57%
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“…It is worthwhile to mention that, if one can neglect PCE, 2p-resonance state locates at Q 2p = h 1 + h 2 = 2ǫ r , where ǫ r is the α − p resonance energy. In this case, where 2p-wave function keeps the pure (p 3/2 ) 2 configuration, it was confirmed that the decay process is well described as a sequential 2p emission [33].…”
Section: Three-body Modelsupporting
confidence: 57%
“…[33], in order to reproduce the resonance energy and width in the (p 3/2 )-channel of α − p scattering, ǫ r = 1.96 MeV and Γ r ≃ 1.5 MeV, respectively [38]. Note that this resonance is attributable to the centrifugal potential barrier [33]. The p − p pairing potential is introduced as…”
Section: Three-body Modelmentioning
confidence: 99%
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