A non-perturbative method [1] which combines constraints from chiral symmet
ry breaking and coupled channel unitarity is used to describe meson-meson i
nteractions up to root s less than or similar to 1.2 GeV, extending in this
way the range of applicability of the information contained in Chiral Pert
urbation Theory (chi PT) [2], since this perturbative series is typically r
estricted to root s less than or similar to 500 MeV. The approach uses the
O(p(2)) and O(p(4)) chi PT Lagrangians. The seven free parameters resulting
from the O(p4) Lagrangian are fitted to the experimental data. The approac
h makes use of the expansion of T-l instead of the amplitude itself as done
in chi PT. The former expansion is suggested by analogy with the effective
range approximation in Quantum Mechanics and it appears to be very useful.
The results, in fact, are in good agreement with a vast amount of experime
ntal analyses [3,4]. The amplitudes develop poles corresponding to the f(0)
(980), a(0)(980), rho(770), K-*(890), the octet contribution to the phi, f(
0)(400 - 1200) - sigma and kappa [4]. The total and partial decay widths of
the resonances are also well reproduced.