Search Results
Search type | Search syntax |
---|---|
Tags | [tag] |
Exact | "words here" |
Author |
user:1234 user:me (yours) |
Score |
score:3 (3+) score:0 (none) |
Answers |
answers:3 (3+) answers:0 (none) isaccepted:yes hasaccepted:no inquestion:1234 |
Views | views:250 |
Code | code:"if (foo != bar)" |
Sections |
title:apples body:"apples oranges" |
URL | url:"*.example.com" |
Saves | in:saves |
Status |
closed:yes duplicate:no migrated:no wiki:no |
Types |
is:question is:answer |
Exclude |
-[tag] -apples |
For more details on advanced search visit our help page |
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 …
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 …