  The quadratic Casimir operator of the special unitary $SU(N)$ group is used
to construct projection operators, which can decompose any of its reducible
finite-dimensional representation spaces contained in the tensor product of two
and three adjoint spaces into irreducible components. Although the method is
general enough, it is specialized to the $SU(2N_f) \to SU(2)\otimes SU(N_f)$
spin-flavor symmetry group, which emerges in the baryon sector of QCD in the
large-$N_c$ limit, where $N_f$ and $N_c$ are the numbers of light quark flavors
and color charges, respectively. The approach leads to the construction of spin
and flavor projection operators that can be implemented in the analysis of the
$1/N_c$ operator expansion. The use of projection operators allows one to
successfully project out the desired components of a given operator and
subtract off those that are not needed. Some explicit examples in $SU(2)$ and
$SU(3)$ are detailed.

High Energy Physics - Phenomenology