\wt\varphi^u_2
v_u/M^2$ and $m_c \approx \varphi^u_2 v_u/M$, are correctly produced, while the top quark mass is of order $v_u$ being generated through a renormalisable operator, see Eq.(\[LOup\]). For small and moderate values of $\tan\beta$, $\tan \beta = v_u/v_d$, $\varphi^d_3 \sim \la^2 M$ gives rise to the correct bottom quark and tau lepton mass. The Cabibbo angle requires $\varphi^d_2 \sim \la \, M$ so that $\theta_C \approx \tilde{x}_2/y_s \la$, see [@HKL10] for details. The correct size of the mass of the strange quark and of the muon is achieved for $\wt\varphi^d_3 \sim \la^3 M$. As one can check, the electron and the down quark mass are also of the correct order of magnitude and the masses of charged leptons and down quarks fulfil the GJ relations [@GJ]. Furthermore, the GST relation holds in the quark sector [@GST]. Eventually, the VEVs $\varphi^\nu_{1,2,3'}$ of the flavons $\Phi^\nu_1$, $\Phi^\nu_2$ and $\Phi^\nu_{3'}$ are of order $\la^4 M$ in order to correctly generate the light neutrino mass scale $m_\nu \sim 0.1 \,
\mathrm{eV}$. The light neutrino mass spectrum can have either hierarchy. In the original model the value of the lepton mixing angle $\theta_{13}^l$ is determined by the mixing in the charged lepton sector [@th13troughth12e] which 