In this Letter we introduce a new model of a diluted Anderson model, which
is a non-trivial generalization of a previous work of Late and Onell (Physi
ca B 299 (2001) 173), because every Anderson impurity is surrounded by two
different sets of site energies, generated by two different periodic functi
ons epsilon (i) = f(i), i =2,...,(l(1) + 1), and epsilon (k) = h(k),k = (l(
1) + 1),..., (l(1) + l(2) + 2). Thus, this disordered model has two interpe
netrating Anderson lattices with the same periodicity P = (l(1) + l(2) + 2)
, where l(1) and l(2) are the numbers of impurities on each diluting set. I
n addition, the distance between two consecutive Anderson impurities altern
ates between l(1) and l(2) values, apparently breaking the spatial correlat
ion, which produces delocalized states when the disorder is diluted in a pe
riodical form. Using the block decimation scheme, we demonstrate the existe
nce of exactly (l(1) + l(2)) Critical energy values for which this disorder
ed system presents delocalized slates. (C) 2001 Elsevier Science B.V, All r
ights reserved.