Bayesian three-body modeling of 22C reveals it is bound by less than 0.35 MeV with s-wave dominance and highlights the need for final-state interactions in dipole strength calculations, with ~50% uncertainties.
Halo Nuclei from Ab Initio Nuclear Theory
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abstract
A realistic description of halo nuclei, characterized by low-lying breakup thresholds, requires a proper treatment of continuum effects. We have developed an ab initio approach, the no-core shell model with continuum (NCSMC), capable of describing both bound and unbound states in light nuclei in a unified way. With chiral two- and three-nucleon interactions as the only input, we can predict structure and dynamics of halo and other light nuclei and, by comparing to available experimental data, test the quality of chiral nuclear forces. We review NCSMC calculations of weakly bound states and resonances of exotic halo nuclei $^6$He, $^8$B, $^{11}$Be, and $^{15}$C. For the latter, we discuss its production in the capture reaction $^{14}$C(n,$\gamma$)$^{15}$C. We highlight challenges of a description of $^6$He as a Borromean n-n-$^4$He system. Finally, we present calculations of excited states in $^{10}$Be exhibiting a one-neutron halo structure and a large scale no-core shell model investigation of $^{11}$Li as a precursor of a full n-n-$^9$Li NCSMC study.
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Uncertainty quantified three-body model applied to the two-neutron halo $^{22}$C
Bayesian three-body modeling of 22C reveals it is bound by less than 0.35 MeV with s-wave dominance and highlights the need for final-state interactions in dipole strength calculations, with ~50% uncertainties.