Kl3 form factors at order p6 of chiral perturbation theory

This paper describes the calculation of the semileptonic K-l3 decay form factors at order p(6) of chiral perturbation theory, which is the next-to-leading order correction to the well-known p(4) result achieved by Gasser and Leutwyler. At order p(6) the chiral expansion contains one- and two-loop diagrams which are discussed in detail. The irreducible two-loop graphs of the sunset topology are calculated numerically. In addition, the chiral Lagrangian L-(6) produces direct couplings with the W bosons. Due to these unknown couplings, one can always add linear terms in q(2) to the predictions of the form factor f(-) (q(2)). For the form factor f(+) (q(2)), this ambiguity involves even quadratic terms. Making use of the fact that the pion electromagnetic form factor involves the same q(4) counterterm, the q(4) ambiguity can be resolved. Apart from the possibility of adding an arbitrary linear term in q(2) our calculation shows that chiral perturbation theory converges very well in this application, as the O(p(6)) corrections are small. Comparing the predictions of chiral perturbation theory with the recent CPLEAR data, it is seen that the experimental form factor f+ (q(2)) is well described by a linear fit, but that the slope lambda(+) is smaller by about 2 standard deviations than the O(p(4)) prediction. The unavoidable q(2) counterterm of the O(p(6)) corrections allows one to bring the predictions of chiral perturbation theory into perfect agreement with experiment.