While the purely leptonic decays are quite easy to understand by just using perturbation theory to the electroweak standard model, QFD, the semi-leptonic decays involving hadrons and the strong interaction, is not so easy to understand from simple analytic principles. An important theoretical tool is to use the approximate chiral symmetry of QCD in the light-quark sector to derive effective hadronic models. Finally there are also some phenomenological models. In connection with the electromagnetic (and maybe also for the weak) interaction of hadrons, particularly pions, the socalled vector-meson-dominance model is quite successful. If I remember right, for the decay via vector and axial-vector currents you need both, direct decays as well as decays vial ##\rho## and ##a_1## mesons. Above, I've quoted a review paper which seems to me pretty up to date concerning ##\tau## physics.