“…[31,32] Recently, permutation symmetric states have received a revived attention in diverse branches of physics due to their geometrical intuition and experimental importance. [13,14,33,34] Dicke states |s, m , the common eigenstates of Ŝ2 , Ŝz belonging respectively to eigenvalues s(s + 1)h 2 , mh, m = −s, −s + 1, . .…”