“…We work in the usual approximation where only the (3, 3) family components, y b , y t , y τ , of each Yukawa couplings matrix are important (for a review of these and other issues, see e.g. [16][17][18]). Concerning the Higgs sector, as common in this kind of phenomenological studies [19,20], we do not choose any specific model for (µ, Bµ), but we treat them as free parameters.…”