By making use of adapted analytic smoothing techniques, we prove that the solutions of Hölder-differentiable Hamiltonian systems, associated to initial conditions in a small ball of radius \(\rho >0\) around a Lagrangian, \((\gamma ,\tau )\) -Diophantine, quasi-periodic torus, are stable over a time \(t^{\text {stab}}\simeq 1/(|\rho |^{1+\frac{\ell -1}{\tau +1}}|\ln \rho |^{\ell -1})\) , where \(\ell >2d+1, \ell \in \mathbb {R}\) , is the regularity, and d is the number of degrees of freedom. In the finitely differentiable case (for integer \(\ell \) ), this result improves the previously known effective stability bounds around Diophantine tori. Moreover, by a previous work based on the Anosov–Katok construction, it is known that for any \(\varepsilon >0\) there exists a \(C^\ell \) -Hamiltonian, with \( \ell \ge 3\) , admitting a sequence of solutions starting at distance \(\rho _n \rightarrow 0\) from a \((\gamma ,\tau )\) -Diophantine torus that diffuse in a time of order \(t^{\text {diff}}_n\simeq 1/(|\rho _n|^{1+\frac{\ell -1}{\tau +1}+\varepsilon })\) . Therefore, for \(\ell >2d+1\) , the stability estimates that we show are optimal up to an arbitrarily small polynomial correction.