In this paper decomposition of periodic orbits in bifurcation diagrams are derived in unidimensional dynamics system xn+1 = f (xn; r), being f an unimodal function. We proof a theorem which states the necessary and sufficient conditions for the break-up of compound orbits in their simpler constituents. A corollary to this theorem provides an algorithm for the computation of those orbits. This process closes the theoretical framework initiated in (Physica D, 239:1135(Physica D, 239: -1146(Physica D, 239: , 2010.