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avito009
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The title says it all.
arivero said:1) Why all the other 21 particles almost massless, respective to the scale of the Higgs Field? Is there some hidden symmetry that should appear when the masses of such particles are all of them (except, as we said, the top quarks) exactly zero.
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lpetrich said:$$ G = g^2 (t_{GUT} - t) $$
So in the limit of low t, y -> g.
I think to remember now that the article of Cecilia Jarlskow with Georgi was also a RG argument.lpetrich said:I don't recall anyone claiming that for any (MS)SM RGE solutions. That's likely because these particles' gauge couplings are usually larger than their Yukawa ones, and when gauge couplings dominate, you get behavior like y ~ tc.
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