Effects of neutron-rich nuclei masses on symmetry energy

Abstract

We explore the impact of neutron-rich nuclei masses on the symmetry energy properties using the mass table evaluated by the deformed relativistic Hartree-Bogoliubov theory in continuum (DRHBc) model. First, using the semi-empirical mass formula with the DRHBc mass table, we investigate the symmetry energy at saturation density ρ0\rho_0, denoted as S0S_0, and the ratio of surface to volume contributions to the symmetry energy, κ\kappa. As a result, we obtain S0=27.85MeVS_0=27.85\,{\rm MeV} (κ=1.38\kappa=1.38) for asym(A)=S0(1κA1/3)a_{\rm sym}(A) =S_0 (1 - \kappa A^{-1/3}) (Type I) and S0=32.66MeVS_0=32.66\,{\rm MeV} (κ=3.15\kappa=3.15) for asym(A)=S0(1+κA1/3)1a_{\rm sym}(A) = S_0 (1 + \kappa A^{-1/3} )^{-1} (Type II), which are lower than those obtained using the AME2020 mass table, S0=28.54MeVS_0=28.54\,{\rm MeV} (κ=1.29\kappa=1.29) for Type I and S0=33.81MeVS_0=33.81\,{\rm MeV} (κ=3.04\kappa=3.04) for Type II. Second, we further investigate the effect of these changes in asym(A)a_{\rm sym}(A) on the density-dependent symmetry energy by employing the empirical model of S(ρ)=Ck(ρ/ρ0)2/3+C1(ρ/ρ0)+C2(ρ/ρ0)γS(\rho) = C_k(\rho/\rho_0)^{2/3} + C_1(\rho/\rho_0) + C_2(\rho/\rho_0)^{\gamma} and universal relation of asym(A=208)=S(ρ=0.1fm3)a_{\rm sym}(A=208) = S(\rho=0.1\,{\rm fm}^{-3}). Compared to the experimental constraints, we find that S0S_0 and slope parameter LL, determined by the DRHBc mass table with Type II, are more suitable to explain the constraints by heavy ion collisions and isobaric analog states than AME2020. We also discuss the neutron skin thickness derived from the LL, comparing it with experimental measurements

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