Electric dipole strength and dipole polarizability in $^{48}$Ca within a fully self-consistent second random-phase approximation

TL;DR

This paper employs a fully self-consistent second random-phase approximation model with subtraction to analyze dipole strength and polarizability in $^{48}$Ca, achieving improved agreement with experimental data over previous models.

Contribution

It introduces a fully self-consistent second RPA model with subtraction for the first time, accurately reproducing dipole strength and polarizability in $^{48}$Ca.

Findings

Accurately reproduces low-lying dipole strength below neutron threshold.

Describes giant dipole resonance with good spreading and fragmentation.

Provides a polarizability curve matching experimental slope around the resonance centroid.

Abstract

The second random-phase-approximation model corrected by a subtraction procedure designed to cure double counting, instabilities, and ultraviolet divergences, is employed for the first time to analyze the dipole strength and polarizability in $^{48}$Ca. All the terms of the residual interaction are included, leading to a fully self-consistent scheme. Results are illustrated with two Skyrme parametrizations, SGII and SLy4. Those obtained with the SGII interaction are particularly satisfactory. In this case, the low-lying strength below the neutron threshold is extremely well reproduced and the giant dipole resonance is described in a very satisfactory way especially in its spreading and fragmentation. Spreading and fragmentation are produced in a natural way within such a theoretical model by the coupling of 1 particle-1 hole and 2 particle-2 hole configurations. Owing to this feature, we may provide for the electric polarizability as a function of the excitation energy a curve with a similar slope around the centroid energy of the giant resonance compared to the corresponding experimental results. This represents a considerable improvement with respect to previous theoretical predictions obtained with the random-phase approximation or with several ab-initio models. In such cases, the spreading width of the excitation cannot be reproduced and the polarizability as a function of the excitation energy displays a stiff increase around the predicted centroid energy of the giant resonance.