In the original model the quark-lepton families fall into the horizontal triplets of the local S U ( 2 ) F symmetry taken. Fortunately, this symmetry is generically free from the gauge anomaly problem which may appear for other local family symmetry candidates. Generally, the model contains the set of the Higgs boson multiplets being scalar, vector and tensor of S U ( 2 ) F , apart from they all are the doublets of the conventional electroweak symmetry S U ( 2 ) W × × U ( 1 ) Y . These scalar multiplets provide the mass matrices for quarks and leptons giving eventually the reasonable weak mixing angles in terms of the fermion mass ratios. In principle, one could hope to reach it in a more economic way when the heavy family masses appears at the tree-level, while the light families acquire their masses from radiative corrections at the one–loop level and higher ones.