What Are the Effects of Zeeman Shift in Positronium?

In summary, the conversation discusses the magnetic moment of an electron and positron, the ground state quantum numbers, the physical mechanism for the Zeeman shift, the Hamiltonian and its components, the possible values for the total spin F in the ground state of positronium, and the energy level shift as a function of applied magnetic field. The g-factor and energy shift equations are also mentioned. The Zeeman effect is explained as the effect on an atom's magnetic moment due to an external magnetic field.
  • #1
QuantumIsHard
3
0

Homework Statement



The magnetic moment for an electron is [itex]\mue = -e/m Se[/itex].
The magnetic moment for a positron is [itex]\mue = +e/m Se[/itex].
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 [itex]H0[/itex] 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:
[itex]gJ = 1 + {j*(j+1) – l*(l+1) + 3/4}/{2*j*(j+1)}[/itex]

Energy shift:
[itex]EZ1 = \muB gJ Bext mJ[/itex]

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) [itex]H0 = -\hbar^2/{2m} * ( {\delta^2}/{\delta^2 r1} ) - \hbar^2/{2m} * ( {\delta^2}/{\delta^2 r2} )[/itex] and [itex]H' = {k*e^2}/{|r1-r2|^2}[/itex], 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 [itex]\muB, gJ, and, mJ[/itex]

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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  • #3
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 [itex]H=\mu\cdot B_{ext}.[/itex] (think about why).
I don't know what you are referring to by H_0 and H'.
 
Last edited:
  • #4
I have given a reference in post#3 there,which deals with both.
 
  • #5




a) The physical mechanism for the Zeeman shift on positronium is the interaction between the magnetic dipole moments of the electron and positron. As the positronium is placed in an external magnetic field, the electron and positron will experience a torque due to their magnetic dipole moments, causing a shift in the energy levels.

b) The Hamiltonian for positronium can be written as H = H0 + H', where H0 is the unperturbed Hamiltonian and H' is the perturbation term. In this case, H0 represents the kinetic energy of the electron and positron, while H' represents the potential energy due to their mutual interaction.

c) In the weak-field limit, the total spin F can take on values of 0 or 1. This is because the electron and positron can either have their spins aligned (F=1) or opposite (F=0).

d) In order to find the g-factor for each value of F, we can use the equation gF = 1 + \frac{F(F+1)-J(J+1)+S(S+1)}{2F(F+1)}, where J is the total angular momentum and S is the total spin. For F=0, we have gF=1, and for F=1, we have gF=2. This means that the energy levels for F=0 will not be shifted in the presence of an external magnetic field, while the energy levels for F=1 will have a Zeeman shift proportional to the external magnetic field.

e) In the weak-field limit, the energy levels for F=1 will be split into three levels, with the middle level being degenerate. This is because the Zeeman shift is proportional to the magnetic field and the energy levels are spaced by the energy difference between the two spin states. For F=0, the energy levels will remain unchanged. The energy level shift can be sketched as a function of the applied magnetic field, with the energy levels for F=1 being shifted upwards and downwards, while the energy levels for F=0 remain unchanged.
 

FAQ: What Are the Effects of Zeeman Shift in Positronium?

1. What is Zeeman shift on Positronium?

Zeeman shift on Positronium is a phenomenon where the energy levels of a Positronium atom are split due to the presence of an external magnetic field. This results in the spectral lines of the atom being shifted, which can be observed through spectroscopy.

2. How does Zeeman shift on Positronium occur?

Zeeman shift on Positronium occurs due to the interaction between the magnetic moment of the atom and the external magnetic field. This interaction leads to a splitting of the energy levels, resulting in a shift in the spectral lines.

3. What is the significance of studying Zeeman shift on Positronium?

Studying Zeeman shift on Positronium can provide valuable insights into the fundamental properties of the atom, such as its magnetic moment. It can also be used to test the validity of theoretical models and to study the behavior of matter and antimatter interactions.

4. How is Zeeman shift on Positronium measured?

Zeeman shift on Positronium is measured using spectroscopic techniques. The spectral lines of the atom are observed in the presence and absence of an external magnetic field, and the difference in the energy levels is used to calculate the Zeeman shift.

5. Can Zeeman shift on Positronium be controlled?

Yes, Zeeman shift on Positronium can be controlled by varying the strength and direction of the external magnetic field. This allows for precise measurements and manipulation of the energy levels and spectral lines of the atom.

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