mixings $0<\sin\theta_{q1,q2,t,b}<1$. The colors codify the size of $y_{cp}^b$, from red corresponding to $y_{cp}^b=0.2$ to blue corresponding to $y_{cp}^b=2\pi$, with intermediate colors interpolating between those values. On the right we show our results for the scan over a smaller region of the parameter space, $0.45\lesssim \sin\theta_b\lesssim0.70$ and $0.25\lesssim \sin\theta_{q2}\lesssim 0.40$. The colors codify the size of $y_{cp}^b$, from red corresponding to $y_{cp}^b=0.3$ to blue corresponding to $y_{cp}^b=1.6$, with intermediate colors interpolating between those values.[]{data-label="figsymdeltag"}](b-puzzle-model9b-deltag_Yukawa_2.eps "fig:"){width=".45\textwidth"} 0.5cm

The value of $\delta g^{b_R}$ is driven by $\sin\theta_b$, whereas $\delta g^{b_L}$ is mostly determined by $\sin\theta_{q2}$. Demanding $0.0075\lesssim \delta g^{b_R}\lesssim 0.0225$ and $0.001\lesssim \delta g^{b_L}\lesssim 0.004$ we obtain $0.45\lesssim \sin\theta_b\lesssim0.70$ and $0.25\lesssim \sin\theta_{q2}\lesssim 0.40$. On the right of Fig. \[figsymdeltag\] we show our results for the fermionic mixings restricted to these intervals. The colors codify the size of the composite bottom Yukawa, $y_{cp}^b$, with red and blue corresponding to $y_{cp}^b=0.3$ and $y_{cp}^b=1.6$, respectively, and intermediate colors interpolating between these extreme values. For $\sin\theta_b$ and $\sin\theta_{q2}$ in these ranges, we find that a small Yukawa is preferred in the bottom sector: $0.3\lesssim y_{cp}^b\lesssim 1$, as can be seen in the plot by the small number of blue points and the large number of almost 