Abstract

Nuclear collective motion provides valuable constraint on the size of neutron-skin thickness and the properties of nuclear matter symmetry energy. By employing relativistic nuclear energy density functional (RNEDF) and covariance analysis related to $\chi^2$ fitting of the model parameters, relevant observables are identified for dipole excitations, which strongly correlate with the neutron-skin thickness $(r_{np})$, symmetry energy at saturation density $(J)$ and slope of the symmetry energy $(L)$. Using the RNEDF framework and experimental data on pygmy dipole strength ($^{68}$Ni, $^{132}$Sn, $^{208}$Pb) and dipole polarizability ($^{208}$Pb), it is shown how the values of $J$, and $L$, and $r_{np}$ are constrained. The isotopic dependence of moments associated to dipole excitations in $^{116-136}$Sn shows that the low-energy dipole strength and polarizability in neutron-rich nuclei display strong sensitivity to the symmetry energy parameter $J$, more pronounced than in isotopes with moderate neutron-to-proton number ratios.

Highlights

  • By employing the relativistic nuclear energy density functional, in this article we explore the underlying structure of low-energy dipole transition strength, and its relations with the symmetry energy parameters (J,L) and rnp in finite nuclei

  • Model calculations of dipole transitions in nuclei based on the relativistic nuclear energy density functional (RNEDF) are realized in terms of relativistic Hartree-Bogoliubov (RHB) model and relativistic quasiparticle random phase approximation (RQRPA) [1]

  • Pygmy dipole strength represents a unique mode of excitation: its strength is governed by coherent low-E2qp neutron configurations and by decoherence of the proton and neutron 2qp configurations which are on the other side relevant for the collectivity of GDR

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Summary

Introduction

The states of the strongest low-energy (E

7.74 MeV neutrons protons
7.74 MeV ISOSCALAR neutrons protons
Findings
Conclusion
Full Text
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