Spin-orbit coupling for positronium

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Aleolomorfo
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Homework Statement


Considering the atom made of an electron and a positron. The spin-orbit Hamiltonian is:
$$H=\frac{e^2}{4\nu^2c^2r^34\pi\epsilon_0}\vec{L}\cdot\vec{S}$$
with ##\vec{L}## the relative angular momentum, with ##\vec{S}## the total spin and ##\mu## the reduced mass. Finding the levels in which ##3d## states are split.

Homework Equations

The Attempt at a Solution


First I show you the way I solved the problem.
$$\vec{J}=\vec{L}+\vec{S}$$
$$\vec{S}\cdot\vec{L} = \frac{J^2-L^2-S^2}{2}$$
So I can rewrite the Hamiltonian:
$$H=A(J^2-L^2-S^2)$$
with ##A## which is equal to al the constants. The splitting in energy is:
$$\Delta E = A\hbar^2 (J(J+1) - \frac{21}{4})$$
In the last step I put ##S=\frac{1}{2}## and ##L=2##. Then I calculate the possible ##J##'s:
$$|L-S|\le J \le L+S$$
So there is a double splitting with ##J=\frac{3}{2}## and ##J=\frac{5}{2}##.

I think the reasoning is right (isn't it?), but I have a question about the spin. I put ##S=\frac{1}{2}## automatically as in the hydrogen spin-orbit coupling. But why do I consider only the spin of the electron and not the total spin of the system, so the spin of the electron and the spin of the positron?
 
on Phys.org
Aleolomorfo said:
I think the reasoning is right (isn't it?), but I have a question about the spin. I put S=12S=12S=\frac{1}{2} automatically as in the hydrogen spin-orbit coupling. But why do I consider only the spin of the electron and not the total spin of the system, so the spin of the electron and the spin of the positron?

The metastable electron-positron bound state can exist in different configurations depending on the relative spin states of the positron and the electron.
These are known as para-positronium (p-Ps), with total spin S = 0 and ortho positronium (o-Ps) with S = 1.
though
These spin states have very different lifetimes

see- the level diagram may help

1. R. Ley, Appl. Surf. Sci. 194 301(2002)
2. http://pyweb.swan.ac.uk/quamp/quampweb/talks/CASSIDY_QuAMP_2013.pdf