For γ > 0, we are interested in blow up solutions u ∈ C + (B) of the fractional problem in the unit ball BWe distinguish particularly two orders of singularity at the boundary: solutions exploding at the same rate than δ 1− α 2 (δ denotes the Euclidean distance) and those higher singular than δ 1− α 2 . As a consequence, it will be shown that the classical Keller-Osserman condition can not be readopted in the fractional setting.