“…The existence of this limit, both P(dω)-a.s. and in L 1 (P), and the fact that f (β, p) is nonrandom are proved in [8] via super-additivity arguments. Notice that trivially Z β, p N ,ω ≥ 1 and hence f (β, p) ≥ 0 for all β, p. Zero is in fact the contribution to the free energy of the paths that never touch the wall: indeed, by restricting to the set of random walk trajectories that stay strictly positive until time N , one has By a standard coupling on the environment, it is clear that the function p → f (β, p) is nondecreasing.…”