24–28 Oct 2022
University of Santiago de Compostela
Europe/Madrid timezone

The kink effect of the nuclear charge radii in some isotopic chains and the nucleon-nucleon tensor force within nonlinear relativistic models in the Hartree-Fock approximation.

Not scheduled
30m
Facultad de Ciencias de la Comunicación (University of Santiago de Compostela)

Facultad de Ciencias de la Comunicación

University of Santiago de Compostela

Campus Norte, Av. de Castelao, s/n, 15782 Santiago de Compostela, Spain
Poster P2 Nuclear Structure, Spectroscopy, and Dynamics P2 Nuclear Structure, Spectroscopy, and Dynamics

Speaker

Prof. Saturnino Marcos (University of Cantabria)

Description

The marked change in trend of the evolution of the charge radii of some isotopic families of nuclei versus the mass number A is known as kink effect. This is a consequence of the shell structure of nuclei and, obviously, cannot be explained by the droplet model. The fact that the density-dependent Hartree-Fock model with standard Skyrme functionals [1] or Gogny forces [2] were not able to reproduce this effect for the lead isotopic chain, for example, whereas the relativistic models in the simple mean-field approach did reasonably well [3,4], has increased the interest in understanding the mechanism responsible for the kink effect [5-12]. However, it seems that the full theoretical understanding has not been reached yet.
The aim of this communication is to use relativistic nonlinear models based on the Hartree-Fock approximation, including the sigma, omega, pi and rho mesons, to explore the influence of the nucleon-nucleon tensor force on the behaviour of the nuclear charge radii of some isotopic chains.
It is found that most of the effect of the tensor force on the nuclear charge radii is channeled, indirectly, through the effect of this force on the spin-orbit splittings. We conclude that the formation of the kink effect in the lead isotopic chain is produced, essentially, by the combination of the binding energy of the 1i11/2 neutron orbital and its geometrical properties, which cannot be reduced to the magnitude of the overlap of its wave function with those of the proton orbitals.
References
[1] N. Tajima, P. Bonche, H. Flocard, P.-H. Heenen, M. S. Weiss, Nucl. Phys. A 551 (1993) 434.
[2] T. Gonzalez-Llarena, J. L. Egido, G. A. Lalazissis, P. Ring, Phys. Lett. B 379 (1996) 13.
[3] M. M. Sharma, G. A. Lalazissis, P. Ring. Phys. Lett. B 317 (1993) 9.
[4] M. M. Sharma, G. A. Lalazissis, J. König, P. Ring. Phys. Rev. Lett. 74 (1995) 3744.
[5] P. G. Reinhard, H. Flocard. Nucl. Phys. A 584 (1995) 467.
[6] S. Marcos, L. N. Savushkin, M. López-Quelle, R. Niembro, P. Bernardos, Phys. Lett. B 507, (2001) 135.
[7] H. De Witte et al., Phys. Rev. Lett. 98 (2007) 112502.
[8] T. E. Cocolios et al., Phys. Rev. Lett. 106 (2011) 052503.
[9] R. Niembro, S. Marcos, M. López-Quelle, L. N. Savushkin, Physics of Atomic Nuclei 75, (2012) 269.
[10] P. M. Goddard, P. D. Stevenson, A. Rios, PRL 110 (2013) 032503.
[11] H. Nakada, T. Inakura, Phys. Rev. C 91 (2015) 021302(R).
[12] H. Nakada, International Journal of Modern Physics E 29 (2020) 1930008.

Primary author

Prof. Saturnino Marcos (University of Cantabria)

Co-authors

Dr Mercedes López-Quelle (University of Cantabria) Dr Ramón Niembro (University of Cantabria)

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