A. Cieplý

Chirally motivated K− nuclear potentials

Abstract In-medium subthreshold K ¯ N scattering amplitudes calculated within a chirally motivated meson–baryon coupled-channel model are used self consistently to confront K − atom data across the periodic table. Substantially deeper K − nuclear potentials are obtained compared to the shallow potentials derived in some approaches from threshold K ¯ N amplitudes, with Re V K − chiral = − ( 85 ± 5 ) MeV at nuclear matter density. When K ¯ N N contributions are incorporated phenomenologically, a very deep K − nuclear potential results, Re V K − chiral + phen . = − ( 180 ± 5 ) MeV , in agreement with density dependent potentials obtained in purely phenomenological fits to the data. Self consistent dynamical calculations of K − –nuclear quasibound states generated by V K − chiral are reported and discussed.

In-medium ηN interactions and η nuclear bound states

{K}^{\ensuremath{-}}

Constraints on the threshold K− nuclear potential from FINUDA ZA(Kstop−,π−)ZΛA spectra

atomic data are used to test several models of the

Coupled channel appooach for pionic atoms 1H and 3He

{K}^{\ensuremath{-}}

Calculations of kaonic nuclei based on chiral meson-baryon coupled channel interaction models

nucleus interaction. The

K− nuclear potentials based on chiral meson-baryon amplitudes

t(\ensuremath{\rho})\ensuremath{\rho}

Testing the K−-nucleus interaction in (Kstop−, τ) reactions

optical potential, due to coupled channel models incorporating the

Low-energy K− optical potentials: deep or shallow?

\ensuremath{\Lambda}(1405)

Study of chirally motivated low-energy K− optical potentials

dynamics, fails to reproduce these data. A standard relativistic mean field (RMF) potential, disregarding the