What are the eigenstates of the anti-ferromagnetic dimer Hamiltonian?

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Homework Help Overview

The problem involves finding the eigenstates and eigenvalues of the Hamiltonian for a simple anti-ferromagnetic dimer, expressed in terms of spin operators. The original poster attempts to understand how to manipulate the Hamiltonian to extract the eigenvalues and eigenvectors.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss rewriting the Hamiltonian in terms of total spin operators and applying spin operator properties to derive the eigenvalues. There are questions about the correctness of the transformations and the resulting expressions.

Discussion Status

Some participants have provided hints and confirmations regarding the manipulation of the Hamiltonian and the nature of the eigenstates. There is an ongoing exploration of the eigenvalues derived from the Hamiltonian, with some participants expressing confidence in their results.

Contextual Notes

The discussion reflects a focus on the mathematical treatment of the Hamiltonian, with specific attention to the implications of the anti-ferromagnetic interactions and the role of external magnetic fields. There is an acknowledgment of the need to derive results consistent with known physical states, such as singlet and triplet states.

opaka
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Homework Statement


The hamiltonian of a simple anti-ferromagnetic dimer is given by

H=JS(1)\bulletS(2)-μB(Sz(1)+Sz(2))

find the eigenvalues and eigenvectors of H.

Homework Equations





The Attempt at a Solution


The professor gave the hint that the eigenstates are of S2=(S(1)+S(2))2, S(1)2, S(2)2, and Sz. So I know I should have four eigenvalues. but I still have no Idea how to get this into a form that I recognize as being able to get eigenvalues from. (a matrix, a DiffEQ, etc.)

Please help
 
Last edited:
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The hint is to help you to deal with the ##\vec{S}_1\cdot\vec{S}_2## term. Rewrite that term in terms of ##\vec{S}^2##, ##\vec{S}_1^2##, and ##\vec{S}_2^2##.
 
When I do that, and apply the spin operators, S2 ket (S,Sz)=s(s+1) ket (s,sz) and Sz ket (S,Sz) = szket (s,sz)(sorry, couldn't find the ket symbol in latex)
I get
H = J/2 (s(s+1) - s1(s1+1)-s2(s2+1))-μB(s1z+s2z)

Is this correct?
 
Yes. Now you can calculate what H does to simultaneous eigenstates of ##\vec{S}^2##, ##S_z##, ##\vec{S}_1^2##, and ##\vec{S}_2^2##. Recall that these are exactly the states that you got from adding angular momenta.
 
I get four answers : J/4 + μB, J/4 -μB, J/4 and - 3J/4. Is this right? These look like the singlet and triplet state energies, but with an added B term.
 
Yeah, that looks right.
 
Thanks so much Vela! you've been a wonderful help.:smile:
 

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