“…Secondly, even for completely random perturbations, if M is finite dimensional, then the leading eigenvalue will be in general outside the unit circle. It is true that as the dimension N of M is increased, the leading eigenvalue tends to the unit circle, but it does so very slowly, possibly like N −1/3 [43]. So, in practice, some finite deviations from the Lyapunov decay rate should not be ruled out.…”