“…Let N ∈ Z + and p ∈ (1, N ) to be given, and let u be a a bounded viscosity solution on (0, T ) × R N to (1), with a Hamiltonian H(t, x, P ) satisfying coercivity property (2). Then, it follows that, for each δ ∈ (0, T ), we have u ∈ C α ([δ, T )×R N ), where α ∈ (0, 1), and u C α ([δ,T )×R N ) depend only on N , δ, Λ, p and u L ∞ ((0,T )×R N ) .…”