The electric dipole strength distribution in Ni58 between 6 and 20 MeV has been determined from proton inelastic scattering experiments at very forward angles at RCNP, Osaka. The experimental data are rather well reproduced by quasiparticle random-phase approximation calculations including vibration coupling, despite a mild dependence on the adopted Skyrme interaction. They allow an estimate of the experimentally inaccessible high-energy contribution above 20 MeV, leading to an electric dipole polarizability αD(Ni58)=3.48(31)fm3. This serves as a test case for recent extensions of coupled-cluster calculations with chiral effective field theory interactions to nuclei with two nucleons on top of a closed-shell system.
Electric dipole polarizability of 58Ni / I. Brandherm, F. Bonaiti, P. von Neumann-Cosel, S. Bacca, G. Colo, G.R. Jansen, L. Z. Z., H. Matsubara, Y.F. Niu, P.-. Reinhard, A. Richter, X. Roca-Maza, A. Tamii. - In: PHYSICAL REVIEW. C. - ISSN 2469-9993. - 111:2(2025 Feb 13), pp. 024312.1-024312.8. [10.1103/physrevc.111.024312]
Electric dipole polarizability of 58Ni
G. Colo;X. Roca-MazaPenultimo
;
2025
Abstract
The electric dipole strength distribution in Ni58 between 6 and 20 MeV has been determined from proton inelastic scattering experiments at very forward angles at RCNP, Osaka. The experimental data are rather well reproduced by quasiparticle random-phase approximation calculations including vibration coupling, despite a mild dependence on the adopted Skyrme interaction. They allow an estimate of the experimentally inaccessible high-energy contribution above 20 MeV, leading to an electric dipole polarizability αD(Ni58)=3.48(31)fm3. This serves as a test case for recent extensions of coupled-cluster calculations with chiral effective field theory interactions to nuclei with two nucleons on top of a closed-shell system.| File | Dimensione | Formato | |
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