Th. A. Rijken
Radboud University Nijmegen
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Featured researches published by Th. A. Rijken.
European Physical Journal C | 1986
E. Van Beveren; Th. A. Rijken; K. Metzger; C. Dullemond; George Rupp; J. E. F. T. Ribeiro
AbstractA unitarized non-relativistic meson model which is successful for the description of the heavy and light vector and pseudo-scalar mesons yields in its extension to the scalar mesons for the same model parameters a complete nonet below 1 GeV. In the unitarization scheme real and virtual meson meson decay channels are coupled to the quark antiquark confinement channels. The flavor dependent harmonic oscillator confining potential itself has bound states ɛ(1.3 GeV),S(1.5 GeV), δ(1.3 GeV), κ(1.4 GeV), similar to the results of other bound stateq
Physical Review C | 1999
V. G. J. Stoks; Th. A. Rijken
Physical Review C | 2014
Y. Yamamoto; T. Furumoto; Nobutoshi Yasutake; Th. A. Rijken
\bar q
Annals of Physics | 1973
M. M. Nagels; Th. A. Rijken; J. J. de Swart
Physical Review C | 1994
R. Timmermans; Th. A. Rijken; J. J. de Swart
models. However, the full coupled channel equations show poles at ɛ(0.5 GeV),S(0.99 GeV), δ(0.97 GeV), κ(0.73 GeV). Not only these pole positions can be calculated in our model also cross sections and phase shifts in the meson scattering channels which are in reasonable agreement with the available data for ππ, ηπ andKπ inS-wave scattering.
Physical Review C | 2006
Th. A. Rijken
SU(3) symmetry relations on the recently constructed hyperon-nucleon potentials are used to develop potential models for all possible baryon-baryon interaction channels. The main focus is on the interaction channels with total strangeness S={minus}2, {minus}3, and {minus}4, for which no experimental data exist yet. The potential models for these channels are based on SU(3) extensions of potential models for the S=0 and S={minus}1 sectors, which {ital are} fitted to experimental data. Although the SU(3) symmetry is not taken to be exact, the S=0 and S={minus}1 sectors still provide the necessary constraints to fix all free parameters. The potentials for the S={minus}2, {minus}3, and {minus}4 sectors, therefore, do not contain any additional free parameters, which makes them among the first models of this kind. Various properties of the potentials are illustrated by giving results for scattering lengths, bound states, and total cross sections. {copyright} {ital 1999} {ital The American Physical Society}
Physical Review C | 2013
Y. Yamamoto; T. Furumoto; Nobutoshi Yasutake; Th. A. Rijken
A multi-Pomeron exchange potential (MPP) is proposed as a model for the universal many-body repulsion in baryonic systems on the basis of the extended soft core (ESC) baryon-baryon interaction. The strength of the MPP is determined by analyzing the nucleus-nucleus scattering with the
Nuclear Physics | 1997
V.G.J. Stoks; Th. A. Rijken
G
Nuclear Physics | 1988
Rob G. E. Timmermans; Th. A. Rijken; J. J. de Swart
-matrix folding model. The interaction in
Physical Review C | 2006
Emiko Hiyama; Toshio Motoba; Y. Yamamoto; Th. A. Rijken
\ensuremath{\Lambda}N