Chee Sheng Fong, Enrico Nardi
A ${\cal G}_{\cal F}=SU(3)_{Q}\times SU(3)_{u}\times SU(3)_{d}$ invariant scalar potential breaking spontaneously the quark flavour symmetry can explain the standard model flavor puzzle and automatically avoids the strong CP problem yielding, at the symmetry breaking minimum, $\theta_{QCD}=0$. The approximate alignment in flavour space of the vacuum expectation values of the up and down `Yukawa fields' is explained as a dynamical effect, and the observed quark mixing angles, the weak CP violating phase, and hierarchical quark masses can be reproduced without introducing hierarchical parameters.
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http://arxiv.org/abs/1307.4412
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