“…Assume that the tail of A ij is such that, for some 0 < α < 2, nP(|A ij | ≥ t) ≃ t→∞ t −α , (in a sense which will be made precise later on). Then, for z ∈ C\R, consider the following fractional moment of the resolvent: For β = 1, as n goes to infinity and then z goes to E ∈ R on the real line, y n z (1)/π converges towards the spectral density which turns out to be positive [7,6,11]. However, we proved in [12] that for β = α/2, and for sufficiently heavy tails (0 < α < 2/3), as n goes to infinity and then z goes to E ∈ R large enough, y n z (α/2) goes to zero.…”