The Dynkin index is additive over a direct sum of group representations, so copies of the fundamental representation have . With , the supplied beta function becomes
For 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.