The classical KAM theorem solves the small-divisor problem when small perturbations are introduced to this function. The partial time derivative of a probability distribution p is given by the Poisson bracket of this function with p. The Legendre transform which transforms from generalized velocity coordinates to conjugate momenta produces it from 
The classical KAM theorem solves the small-divisor problem when small perturbations are introduced to this function. The partial time derivative of a probability distribution p is given by the Poisson bracket of this function with p. The Legendre transform which transforms from generalized velocity coordinates to conjugate momenta produces it from the Lagrangian. The time- independent Schrödinger equation is an eigenvalue equation for, for ten points, what operator, the observable corresponding to the total energy?
The classical KAM theorem solves the small-divisor problem when small perturbations are introduced to this function.
{Hamiltonian}