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A notional even-dimensional space representing all relevant states of a dynamical system; it normally consists of all components of position and momentum/velocity involved in that unique specification. Use for both classical and quantum physics.

2 votes
1 answer
186 views

Perelomov coherent states for an arbitrary Hamiltonian

I'm reading about Perelomov coherent states, but I'm not sure if I'm getting it right. From this question and some Perelomov papers I understand the following: The Perelomov coherent states are gener …
2 votes

Can I swap quantum mechanical ground state for some classical trajectory distribution and ha...

If you take the Liouville equation and set $\frac{\partial \rho}{\partial t} = 0$, so that the probability density doesn't depend on the time, you get (in one dimension): $$\frac{\partial \rho}{\part …
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2 votes
2 answers
566 views

Action variables in canonical transformations

Let's suppose we have a Hamiltonian $H(p_k, q_k)$ and we want to transform it via a canonical transformation to one Hamiltonian which doesn't depend on the new coordinates $w_k$, but only in the momen …
2 votes

Action variables in canonical transformations

I've come up with another answer. The type II generating function $S^\prime(q, J)$ can be obtained from its differential as: $\int dS^\prime = \int p dq + \int w dJ$ But since $J$ is constant, the …
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