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Well working with the dynkin diagram of SU(5), one can easily see (by Dynkin's rule) that possible choices of SU(5) spontaneous symmetry breaking could be:
SU(5)→ SU(4) \times U(1) I call the broken group G
and
SU(5)→ SU(3) \times SU(2) \times U(1) which I call SM
So I have a question. Apart from the natural imposition of the SM subgroup (since we know that this is the gauge symmetry of our below GUT scale physics) is there any particular way the nature could have chosen it to G?
If you understood the question so far, don't procceed I'll try to make it clearer. I would expect that both G and SM are equally possible candidates, but something must have been there to choose the Standard Model to G... what is that something?
Thanks
SU(5)→ SU(4) \times U(1) I call the broken group G
and
SU(5)→ SU(3) \times SU(2) \times U(1) which I call SM
So I have a question. Apart from the natural imposition of the SM subgroup (since we know that this is the gauge symmetry of our below GUT scale physics) is there any particular way the nature could have chosen it to G?
If you understood the question so far, don't procceed I'll try to make it clearer. I would expect that both G and SM are equally possible candidates, but something must have been there to choose the Standard Model to G... what is that something?
Thanks