Abstract. In this review, we will discuss the results of our recent work [1] to study the general optimization of the pure isovector parameters of the popular relativistic mean-field (RMF) and Skyrme-Hartree-Fock (SHF) nuclear energy-density functionals (EDFs), using constraints on the pure neutron matter (PNM) equation of state (EoS) from recent ab initio calculations. By using RMF and SHF parameterizations that give equivalent predictions for ground-state properties of doubly magic nuclei and properties of symmetric nuclear matter (SNM) and PNM, we found that such optimization leads to broadly consistent symmetry energy J and its slope parameter L at saturation density within a tight range of σ(J) < 2 MeV and σ(L) < 6 MeV. We demonstrate that a clear model dependence shows up (a) in the curvature parameter of the symmetry energy K sym , (b) the symmetry energy at supra-saturation densities, and (c) the radius of neutron stars.
IntroductionPhenomenological nuclear effective interactions offer a compact description of the in-medium nucleon-nucleon interaction and are useful tools in the applications of both the nuclear structure and the astrophysical phenomena. The effective interaction is typically dependent on few parameters representing, for example, coupling constants, which are often fit to well-determined experimental nuclear observables such as binding energies, charge radii, single particle energy spectra and spectra of collective excitations. One of the main objective of modern nuclear manybody theory is to obtain an EDF [2] with clear physical connections to ab initio nucleon-nucleon interactions and QCD.In the recent years, much effort has been devoted to constrain the energy per neutron of PNM (E PNM ) at sub-saturation densities. By studying the universal behavior of resonant Fermi gases with infinite scattering length, a significant constraint is achieved for the EoS of dilute neutron matter [3]. These calculations have been extended to higher densities using the full power of quantum Monte Carlo methods [4,5]. Moreover, by studying the physics of chiral threenucleon forces the EoS of PNM is obtained perturbatively up to nuclear saturation density [6]. Finally, the auxiliary field diffusion Monte Carlo (AFDMC) technique, which takes into account the realistic nuclear Hamiltonian containing modern two-and three-body interactions of the