This paper is devoted to the study of P-regularity of viscosity solutions u(x, P), P ∈ R n , of a smooth Tonelli Lagrangian L : T T n → R characterized by the cell equation H (x, P + D x u(x, P)) = H (P), where H : T * T n → R denotes the Hamiltonian associated with L and H is the effective Hamiltonian. We show that if P 0 corresponds to a quasi-periodic invariant torus with a non-resonant frequency, then D x u(x, P) is uniformly Hölder continuous in P at P 0 with Hölder exponent arbitrarily close to 1, and if both H and the torus are real analytic and the frequency vector of the torus is Diophantine, then D x u(x, P) is uniformly Lipschitz continuous in P at P 0 , i.e., there is a constant C > 0 such that D x u(·, P) − D x u(·, P 0 ) ∞ ≤ C P − P 0 for P − P 0 1. Similar P-regularity of the Peierls barriers associated with L(x, v) − P, v is also obtained.