“…We also point out that, in the nonsingular case α 1 = β 2 = 0, the required properties on ζ 1 (and analogously for ζ 2 ) appearing in (3) guarantee that the right-hand side of (1) belongs to L r (R N ), r > N p , which is the minimum requirement (among Lebesgue spaces) on the right-hand side of the p-Poisson equation −∆ p w = h(x) to get w ∈ L ∞ (R N ), making condition (3), in a certain sense, natural. The prototype of (1), obtained by setting γ i = δ i = 0 and m i = M i , has a cooperative structure, i.e., f is increasing in v and g is increasing in u; however, we require no monotonicity assumptions on f, g. The Dirichlet version of (1) in bounded domains has been investigated in [2], while [12] deals with (1) for α 2 = β 1 = 0 and without convection terms (i.e., terms depending on the gradient of solutions). The present investigation follows the direction of the recent papers [11,9,8], regarding singular convective problems in bounded domains, with different boundary conditions.…”