What Are the Effects of Zeeman Shift in Positronium?

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Homework Help Overview

The discussion revolves around the effects of the Zeeman shift in positronium, focusing on the magnetic moments of the electron and positron, the Hamiltonian formulation, and the implications of spin coupling in a magnetic field.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants explore the physical mechanism behind the Zeeman shift and its relation to the magnetic moments of the particles involved. Questions arise regarding the formulation of the Hamiltonian, particularly the definitions of H0 and H'. There is also discussion about the possible values of total spin F in the weak-field limit and how to express the Hamiltonian in terms of F.

Discussion Status

Some participants have provided references and suggestions for further reading, while others have pointed out potential misunderstandings regarding the distinction between hyperfine splitting and the Zeeman effect. The conversation is ongoing, with various interpretations and approaches being explored.

Contextual Notes

The original poster expresses uncertainty about several aspects of the problem and seeks assistance, indicating a lack of confidence in their understanding of the concepts involved.

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Homework Statement



The magnetic moment for an electron is \mu<sub>e</sub> = -e/m S<sub>e</sub>.
The magnetic moment for a positron is \mu<sub>e</sub> = +e/m S<sub>e</sub>.
In the ground state, the quantum numbers are n=1 and l=0.

a) What is the physical mechanism for the Zeeman shift?
b) Write the Hamiltonian and identify H<sub>0</sub> and H'.
c) In the weak-field limit, the two spins couple together to make a total spin F. What are the possible values for F in the ground state of positronium?
d) Continuing in the weak field limit, the Hamiltonian needs to be written in terms of the total spin F. Project each of the spins S onto the total spin F and find the value of the Lande g-factor for each value of F.
e) Sketch the energy level shift as a function of applied B for each value of F in the weak field limit.

Homework Equations



g-factor:
g<sub>J</sub> = 1 + {j*(j+1) – l*(l+1) + 3/4}/{2*j*(j+1)}

Energy shift:
E<sub>Z</sub><sup>1</sup> = \mu<sub>B</sub> g<sub>J</sub> B<sub>ext</sub> m<sub>J</sub>

The Attempt at a Solution



a) The motion of the electron and positron will produce a magnetic field experienced by the other. The Zeeman shift will factor in this field.

b) H0 = -\hbar^2/{2m} * ( {\delta^2}/{\delta^2 r1} ) - \hbar^2/{2m} * ( {\delta^2}/{\delta^2 r2} ) and H&#039; = {k*e^2}/{|r1-r2|^2}, with H just being the sum of the two.

c) F=1 when the spins align and F=0 when the spins are opposite.

d) If I knew j and mj, I believe I could do this with a Clebsh-Gordan table.

e) I think I could just use the above equation once I know \mu<sub>B</sub>, g<sub>J</sub>, and, m<sub>J</sub>

I'm nowhere near confident with (a)-(c) and am stuck entirely on (d) and (e). Any help would be greatly appreciated.

This is my first post on this forum, so my apologies for any formatting issues.
 
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You are explaining hyperfine splitting not the Zeeman effect. The Zeeman effect is the effect on the atom's magnetic moment due to an external magnetic field.

For part b, you can write the hamiltonian as H=\mu\cdot B_{ext}. (think about why).
I don't know what you are referring to by H_0 and H'.
 
Last edited:
I have given a reference in post#3 there,which deals with both.
 

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