I believe this is a simple question, however I cannot find it explained anywhere what the term:
"Impose canonical commutation relations" means.
If I have a classical equation, and I wish to quantise it, I will first promote the classical coordinates to operators, nothing more than notation change. What is the process to then impose the commutation relations for the operators that I have promoted the coordinates to?
For example, if I have a classical Hamiltonian for the harmonic oscillator, and I want to quantise it, how will the Hamiltonian change other than putting hats onto the coordinates, and is the method the same for any Hamiltonian?
– Sean Dec 05 '15 at 10:44