What are the Eigenvalues and Eigenkets of a Spin-1/2 System in a Magnetic Field?

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Homework Help Overview

The discussion revolves around a spin system involving noninteracting spin 1/2 particles subjected to magnetic fields. The original poster is tasked with finding the eigenvalues and eigenkets of the Hamiltonian, which includes terms related to the Pauli spin operators and the applied magnetic fields.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to derive the eigenvalues and eigenkets of the Hamiltonian and expresses uncertainty about their calculations in parts a and b. They seek confirmation on their approach and inquire about potential mistakes.
  • Some participants question the original poster's understanding of the eigenvalue problem and suggest writing the Hamiltonian in matrix form to facilitate solving the eigenvalue equation.
  • Others suggest using a linear combination of the basis kets |+> and |-> to express the eigenstates of H, prompting further exploration of the coefficients involved.

Discussion Status

The discussion is ongoing, with participants providing guidance on different approaches to the problem. There is an exploration of various interpretations regarding the eigenvalue problem and the matrix representation of the Hamiltonian. No explicit consensus has been reached, but several productive directions have been suggested.

Contextual Notes

There is mention of the original poster's unfamiliarity with the matrix form of Pauli matrices, which may impact their ability to proceed with the problem. Additionally, the discussion reflects a lack of coverage of certain topics in the original course, which may constrain the participants' approaches.

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Homework Statement


Consider a spin system with noninteracting spin 1/2 particles. The magnetic moment of the system is written as:
μ = (ħq/2mc)σ
Where σ = (σx, σy, σz) is the Pauli spin operator of the particle. A magnetic field of strength Bz is applied along the z direction and a second field Bx is applied along the x direction. The Hamiltonian of the particles is:
H = H0 + V
H0 = -μzBz
V = -μxBx
a) Find the eigenvalues and eigenkets of H0
b) Express V in terms of σ+ and σ-
c) Find the eigenvalues and eigenkets of H

Homework Equations


σ+ = σx + iσy
σ- = σx - iσy
σ+ = |+><-|
σ- = |-><+|
σz|+> = 1|+>
σz|-> = -1|->

The Attempt at a Solution


For part a) I'm pretty sure I did it right
H0 = (-qBzħ/2mc)σz or H0 = ε0σz if ε0 = -qBzħ/2mc.
The operators H0 and σz commute so they have the same eigenkets |+> and |->
Using the expression for H0 and the eigenvalue equations for σz given above the eigenkets of H0 are ε0 and -ε0.
Part b I'm not so sure. I wrote the expression for V in the same way that I did for H0:
V = (-qBxħ/2mc)σx
Then using equations given above I worked out that σx = (σ+ + σ-)/2, so I subbed that into the the expression to get:
V = (-qBxħ/4mc)(σ+ + σ-)
When I try to do part c I start running into problems and I think it is because I did something in part a or b wrong. Can anyone tell me if I've made any mistakes in part a or b?
 
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phys-student said:
V = (-qBxħ/4mc)(σ+ + σ-)
That looks right.
phys-student said:
I start running into problems
What are your problems?
 
When I try to find the eigenvalues of H I get the expression:

(-ε0σz - (qBxħ/4mc)(σ+ + σ-))|+> = ε|+>

and I don't know how to evaluate it properly. I tried plugging these in: σ+ = |+><-|, σ- = |-><+| but I have no idea what to do after that. Are you supposed to expand it so that you're taking the eigenvalue of the first term and the eigenvalues of the second term?
 
Write the matrix form of ##H## using the knowledge of the matrix form of Pauli matrices. Then solve the eigenvalue problem in resulting matrix equation.
 
I'm not very familiar with the matrix form of Pauli matrices, it wasn't covered in this course... Do you know of a source I can read that would help?
 
There is an alternative route to the solution. You know that the |+> and |-> kets for a complete basis, therefore the eigenstates of H can be written as a|+> + b|->. Try solving H (a|+> + b|->) = E (a|+> + b|->) for a and b (along with proper normalization).
 
Pauli matrices are related to the spin matrices of spin 1/2 particles. But if you are not yet familiar with those matrices, DrClaude's suggestion above will also do the job.
 

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