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Dear Leo Vuyk, to your first question: it is possible
As for your second question: are you absolutely right.
I'm still studying, as it breaks the symmetry of the Higgs vacuum, for, as you well said, oscillate and give mass to the fermions.
I've made some progress, which in summary, is the expose, for if your interest.
What is clear, that is for sure is that the sum of the spins, as I have argued in the essay, it should be considered only the spin 1/2, of the fermions. Since, at the moment focusing on the six leptons, the sum of the spins:
[math]6\cdot{\displaystyle \sum_{s=1/2}(s+1)s=(9/2)}
[/math]
Now, as you well said, the Higgs vacuum oscillation; corresponds, taking into account the electric charges, all (note the equivalences, very important), and the contribution due to Higgs boson:
[math]
10\cdot\bigl\{[\ln(mv(H)/m_{e})-{\displaystyle \sum_{s}(s+1)s}]/7\bigr\}=O_{1}
[/math]
[math]10\equiv|3(\frac{4}{3})|+|3(\frac{2}{3})|+|3(\frac{-1}{3})|+|3(\frac{1}{3})|+|1|+|-1|\equiv2{\displaystyle \sum_{s}s\equiv10d}
[/math]
Clearly, three, by the three colors QCD
[math]7=3(\frac{4}{3})+3(\frac{2}{3})+3(\frac{-1}{3})+3(\frac{1}{3})+1\equiv7d[/math]
1)
[math]6\cdot{\displaystyle \sum_{s=1/2}(s+1)s+O_{1}=(9/2)+O_{1}\simeq\ln(m_{\mu}/m_{e})}
[/math]
2)
[math]2\cdot6\cdot{\displaystyle \sum_{s=1/2}(s+1)s-O_{1}=2\cdot(9/2)-O_{1}\simeq\ln(m_{\tau}/m_{e})}
[/math]
The previous two equations must be met, these two oscillations Higgs vacuum, to preserve the symmetry of the sum of the spins, compared to the sum of the spines (module), the quarkcounting three color charges.
3)
[math]6\cdot{\displaystyle \sum_{s=1/2}(s+1)s+O_{1}+2\cdot6\cdot{\displaystyle \sum_{s=1/2}(s+1)s-O_{1}=3_{C}\cdot6}}\sum_{s=1/2}(s+1)s