Matrix representation of the time operator

In quantum mechanics the time operator \Theta satisfies the commutation relation [\Theta,H]=i, and thus it may be thought of as being canonically conjugate to the Hamiltonian H. The time operator associated with a given Hamiltonian H is not unique because one can replace \Theta by \Theta+ \Theta_{\rm hom}, where $\Theta_{\rm... Show more