“…One derives the expression of S (ℓ) extending the formulation reported in Ref. [5] for spin 1 2 systems to general spin j systems. Specifically, S (ℓ) and S † (ℓ) are expressed in terms of the spin j representations of the generators J − and J + = J † − of the su(2) algebra {J + , J − , J z }, [J + , J − ] = 2J z , [J z , J ± ] = ±J ± , the standard basis |j, m , −j ≤ m ≤ j, being replaced with the number basis through the Holstein-Primakoff representation of su(2) [10].…”