“…Then it follows from [2, Theorem 9] that there exists a unique equilibrium state µ i for (f, Φ i ) which is a weak Gibbs measure with respect to the family of potentials Φ i , for i = 1, 2. Moreover, from [36,Example 4.6], for any c > 0 the tail of the convergence to the largest or smallest Lyapunov exponent (corresponding respectively to j = 1 or j = 2)…”