Speaker
Prof.
Jiri Mares
(Nuclear Physics Institute)
Description
We report on our very recent self-consistent calculations of $K^-$-nuclear quasi-bound states [1]. Relevant $K^-$ optical potentials were developed within several chiral meson-baryon coupled-channel interaction models [2-5]. The applied models yield quite different $K^-$ binding energies and widths [6]. Then, the $K^-$ multinucleon interactions were incorporated by a phenomenological optical potential introduced recently to achieve good fits to kaonic atom data [7].
Our calculations show that the effect of $K^-$ multinucleon interactions on $K^-$ widths in nuclei is decisive. The resulting widths are considerably larger than corresponding binding energies. Moreover, when the density dependence of the $K^-$ multinucleon interactions derived in the fits of kaonic atoms is extended to the nuclear interior, the only two models acceptable after imposing as additional constraint the single-nucleon fraction of $K^-$ absorption at rest do not yield any kaonic nuclear bound state in majority of considered nuclei.
[1] J. Hrtankova, J. Mares, Phys. Lett. B in print, arXiv:1703.01788v2 [nucl-th].
[2] A. Cieply, J. Smejkal, Nucl. Phys. A 881 (2012) 115.
[3] Y. Ikeda, T. Hyodo, W. Weise, Nucl. Phys. A 881 (2012) 98.
[4] Z. H. Guo, J. A. Oller, Phys. Rev. C 87 (2013) 035202.
[5] M. Mai, U.-G. Meissner, Nucl. Phys. A 900 (2013) 51.
[6] J. Hrtankova, J. Mares, subm. Phys. Rev. C, arXiv:1704.07205
[nucl-th].
[7] E. Friedman, A. Gal, Nucl. Phys. A 959 (2017) 66.
Primary author
Ms
Jaroslava Hrtankova
(Nuclear Physics Institute, Rez, Czech Republic)
Co-author
Prof.
Jiri Mares
(Nuclear Physics Institute)