Spin-orbit coupling for positronium

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SUMMARY

The discussion focuses on the spin-orbit coupling in positronium, represented by the Hamiltonian $$H=\frac{e^2}{4\nu^2c^2r^34\pi\epsilon_0}\vec{L}\cdot\vec{S}$$, where $$\vec{L}$$ is the relative angular momentum and $$\vec{S}$$ is the total spin. The energy splitting for the 3d states is derived as $$\Delta E = A\hbar^2 (J(J+1) - \frac{21}{4})$$, leading to double splitting with $$J=\frac{3}{2}$$ and $$J=\frac{5}{2}$$. The discussion also clarifies the distinction between the spin states of para-positronium (p-Ps) with total spin S = 0 and ortho-positronium (o-Ps) with S = 1, emphasizing their different lifetimes.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly angular momentum
  • Familiarity with spin-orbit coupling concepts
  • Knowledge of positronium and its properties
  • Basic proficiency in Hamiltonian mechanics
NEXT STEPS
  • Study the implications of spin states in quantum systems, focusing on para-positronium and ortho-positronium
  • Explore advanced quantum mechanics texts covering spin-orbit coupling in detail
  • Investigate experimental methods for observing positronium states
  • Learn about the applications of positronium in material science and particle physics
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Physicists, quantum mechanics students, and researchers interested in particle physics and the properties of exotic atoms like positronium.

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?
 
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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
 

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