Abstract
The problem of the K+-nucoleon scattering is treated with the method of Tamm-Dankoff in the two-meson approximation, both with scalar and pesudovector coupling. In both cases it turns out that the most important phase at low energy is T=1, which corresponds, to an attractive potential. In the scalar case this phase does not lead to a resonance; in the pseudoscalar case there is, however, a resonant state whose position, is strongly dependent on the momentum cut-offK. At the end of the work there is a brief discussion of the results obtained, in relation to the few experimental data so far available.
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