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Two-nucleon emitters within a pseudostate method: The case of 6^6Be and 16^{16}Be

Published 4 Jan 2018 in nucl-th | (1801.01280v3)

Abstract: Background: Since the first experimental observation, two-nucleon radioactivity has gained renewed attention over the past fifteen years. The <sup>6<sup>6Be system is the lightest two-proton ground-state emitter, while <sup>16<sup>{16}Be has been recently proposed to be the first two-neutron ground-state emitter ever observed. A proper understanding of their properties and decay modes requires a reasonable description of the three-body continuum. Purpose: Study the ground-state properties of <sup>6<sup>6Be and <sup>16<sup>{16}Be within a general three-body model and investigate their nucleon-nucleon correlations in the continuum. Method: The pseudostate (PS) method in hyperspherical coordinates, using the analytical transformed harmonic oscillator (THO) basis for three-body systems, is used to construct the <sup>6<sup>6Be and <sup>16<sup>{16}Be ground-state wave functions. These resonances are approximated as a stable PS around the known two-nucleon separation energy. Effective core-NN potentials, constrained by the available experimental information on the binary subsystems <sup>5<sup>5Li and <sup>15<sup>{15}Be, are employed in the calculations. Results: The ground state of <sup>16<sup>{16}Be is found to present a strong dineutron configuration, with the valence neutrons occupying mostly an l=2l=2 state relative to the core. The results are consistent with previous RR-matrix calculations for the actual continuum. The case of <sup>6<sup>6Be shows a clear symmetry with respect to its mirror partner, the two-neutron halo <sup>6<sup>6He: The diproton configuration is dominant, and the valence protons occupy an l=1l=1 orbit. Conclusions: The PS method is found to be a suitable tool in describing the properties of unbound core+N+N\text{core}+N+N ground states. For both <sup>16<sup>{16}Be and <sup>6<sup>6Be, the results are consistent with previous theoretical studies and confirm the dominant dinucleon configuration. This favors the picture of a correlated two-nucleon emission.

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