00:01
Okay, so we have three spin -1 particles that are placed at the corners of a triangle.
00:04
But what really matters is they give us the hamiltonian, and it looks like this.
00:08
So these are non -interacting, except for the fact that they're spin -1 particles.
00:15
So i'm going to calculate the following quantity.
00:20
So i'm going to call j the total angular momentum.
00:24
It's s1 plus s2 plus s3.
00:30
And let's calculate j squared.
00:58
All of our s's are spin 1, and j gives me j values of 0, 1, 2, or 3.
01:16
And if i take my h now, i hit it on any state j, m.
01:25
And of course, m doesn't matter.
01:26
We're not even thinking about m really.
01:29
But that's going to be...
01:31
So s1, each one of these is spin 1.
01:38
So they get an h bar squared times 1 times 2...