Barton, MatthewStevenson, Paul D.Ríos Huguet, Arnau2022-07-042022-07-042021-06-042469-9985https://hdl.handle.net/2445/187282Background: Time-dependent techniques in nuclear theory often rely on mean-field or Hartree-Fock descriptions. Beyond-mean-field dynamical calculations within the time-dependent density matrix (TDDM) theory have often invoked symmetry restrictions and ignored the connection between the mean field and the induced interaction. Purpose: We study the ground states obtained in a TDDM approach for nuclei from A=12 to A=24, including examples of even-even and odd-even nuclei with and without intrinsic deformation. We overcome previous limitations using three-dimensional simulations and employ density-independent Skyrme interactions self-consistently. Methods: The correlated ground states are found starting from the Hartree-Fock solution, by adiabatically including the beyond-mean-field terms in real time. Results: We find that, within this approach, correlations are responsible for ≈4-5 % of the total energy. Radii are generally unaffected by the introduction of beyond-mean-field correlations. Large nuclear correlation entropies are associated with large correlation energies. By all measures, 12C is the most correlated isotope in the mass region considered. Conclusions: Our work is the starting point of a consistent implementation of the TDDM technique for applications into nuclear reactions. Our results indicate that correlation effects in structure are small, but beyond-mean-field dynamical simulations could provide insight into several issues of interest.application/pdfeng(c) American Physical Society, 2021Física nuclearTeoria del funcional de densitatNuclear physicsDensity functionalsinfo:eu-repo/semantics/article7214472022-07-04info:eu-repo/semantics/openAccess