“…In a diagram I λ versus E λ , the array of (2σ + 1) 2 points form a regular pattern, which, however, is likely to be visually distorted due to the generally complicated nonlinear dependence of E and I on J 1 , J 2 . But we do not, in fact, need to know the 2 nd integral of the motionÎ explicitly to carry out this scheme; we can, following an idea of Peres [24], always construct it via time averages similar to the procedure previously employed for the classical model [18]: Take any operator with [Â,Ĥ] = 0, which represents a dynamical variable independent ofĤ, and consider the matrix elementsÂ(t) in the energy representation,…”