The Dynkin index is additive over a direct sum of group representations, so copies of the fundamental representation have . With , the supplied beta function becomesFor positive gauge coupling , asymptotic freedom at this order requires , hence . For nonnegative integer ,At the one-loop coefficient vanishes, so this formula alone does not establish asymptotic freedom. This count follows the scalar multiplicity convention of the printed beta function; changing how a real or complex scalar field is counted requires changing its coefficient too.
The two-index symmetric representation of SU(3) is , with Dynkin index . Thus copies have , and the supplied beta function isThe strict sign condition for asymptotic freedom is , givingIndeed , while .
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