“…with initial conditions u(0, π) k,l = u 0 (π ) k,l and u t (0, π) k,l = u 1 (π ) k,l , for all π ∈ G and for any k, l ∈ N, where now f (t, π) k,l can be regarded as the source term of the second order differential equation as in (12). Now, let us decouple the matrix equation in (12) by fixing π ∈ G, and treat each of the equations represented in (12) individually. If we denote by…”