“…Even, for relevant classes of operators, each point of the lattice corresponds exactly to one of eigenvalues, counted according to the multiplicity, and the computation of N (λ) leads in a natural way to problems of number theory. Let us refer for example to [8,9], [12]- [22], [28]- [32]. In this order of ideas, the attention will be fixed here on operators of the form of tensor products (1.1) P = P 1 ⊗ ... ⊗ P p where the operators P j , j = 1, .…”