  We study the S-wave kaon-nucleon interactions for strangeness S=-1 in a novel
relativistic chiral unitary approach based on coupled channels. Dispersion
relations are used to perform the necessary resummation of the lowest order
relativistic chiral Lagrangian. A good description of the data in the K^- p,
\pi \Sigma and \pi \Lambda channels is obtained. We show how this method can be
systematically extended to higher orders, emphasizing its applicability to any
scenario of strong self-interactions where the perturbative series diverges
even at low energies. Discussions about the differences to existing approaches
employing pseudo-potentials in a regulated Lippmann-Schwinger equation are
included. Finally, we describe the resonance content of our meson-baryon
amplitudes and discuss its nature.

High Energy Physics - Phenomenology;Nuclear Theory