What Are the Eigenvalues and Eigenvectors of This Spin Hamiltonian?

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Homework Help Overview

The discussion revolves around finding the eigenvalues and eigenvectors of a Hamiltonian operator related to two spin-1/2 particles in quantum mechanics. The original poster expresses confusion regarding the application of the Hamiltonian and the interpretation of the triplet and singlet states.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to understand the eigenvalues and eigenvectors of the given Hamiltonian, referencing solutions provided by a teacher. They question the nature of the triplet states and how to interpret the eigenvalues.
  • Another participant raises a question about the symmetry of the eigenstates for fermions, suggesting that the singlet state should be considered instead of the triplet state.
  • Further inquiries are made regarding the calculation of the Hamiltonian's action on specific states, particularly in relation to the singlet state.

Discussion Status

Contextual Notes

Participants are preparing for an exam and are grappling with the implications of the Hamiltonian's structure and the properties of spin states. There is a noted lack of clarity regarding the definitions and calculations involved.

dreamspy
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Homework Statement



I'm struggling with this question here from my QM class. I have read all my material on Spin (both Griffiths, and a chapter in an Icelandic book). I'we done some problems, but I really have no Idea where to start with this one. It goes something like this:

Two particles have spin 1/2 and are stationary, but their spins interact with this Hamilton operator:

\hat H = \gamma \hat S_3^{(1)} + \gamma \hat S_3^{(2)}

where \bf{S}^{(j)} is the spin operator for particle j, and j=1,2.

As a basis in the state space (hope that's the right word) you can f.x. take u_s^{(1)}u_r^{(2)} wherer,s,=\pm\frac{1}{2}, and \hat S_3^{1}u_s^{1}=shu_s^{j} and \hat S_3^{2}u_r^{2}=rhu_r^{j}

Questions:
(i) Find the eigenvalues and eigenvektors of the Hamilton operator.

(ii) How would the result be if we used this Hamilton operator instead:

\hat H = \gamma \hat S_3^{(1)} + \gamma \hat S_3^{(2)} + \lambda \hat{\underline S}^{(1)}\cdot \lambda \hat{\underline S}^{(2)}

The Attempt at a Solution



Now here is a quick solution I got from my teacher:

(i)
Triplet:


u_{\frac{1}{2}}u_{\frac{1}{2}}
(u_{\frac{1}{2}}u_{-\frac{1}{2}}+u_{-\frac{1}{2}}u_{\frac{1}{2}})\frac{1}{\sqrt 2}
u_{-\frac{1}{2}}u_{-\frac{1}{2}}

\underlince{\hat S}^2 = s(s+1)

The Eigenvalues:

(\gamma S_3^{(1)}-\gamma S_3^{(2)})u_{\frac{1}{2}}u_{\frac{1}{2}} = \gamma \hbar(s+r)u_{\frac{1}{2}}u_{\frac{1}{2}}
(the others should follow the same procedure)

(ii)
Two spin operators:

\underline{\hat S}^{(1)}, \underline{\hat S}^{(2)}

\underline{\hat S}^{(1)}\cdot \underline{\hat S}^{(2)} = \frac{1}{2}(\underline{\hat S}^{2}-(\underline{\hat S}^{(1)})^2-(\underline{\hat S}^{(1)})^2)

\underline{\hat S} = \underline{\hat S}^{(1)} + \underline{\hat S}^{(2)}<br />

\underline{\hat S}} has eigenvalue s(s+1) \hbar ^2, s=0,1


Now I almost have no clue on what's going on here.

Now I suppose the part in the Triplet section, is all possible linear combinations of the u vektors. And the eigenvalue can be read from the right side of the formula below. But could anyone care to comment on this? I'm standing on very shaky ground here :) This is the solution my teacher gave us, nobody has a clue what's going on, and were taking the exam tomorrow :)


Thanks in advance for any comments!
Frímann
 
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My basic quesion is probably, how do I choose the part in the Triplet section, are those the eigenfunctions? If not then how would I find them?
 
Well if I am not mistaken for two fermions the eigenstate should be anti symmetrical, i.e singlet and not triplet which is symmetric.

But I myself in a shaky ground... :-)
 
\underline{\hat S}^{(1)}\cdot \underline{\hat S}^{(2)} = \frac{1}{2}(\underline{\hat S}^{2}-(\underline{\hat S}^{(1)})^2-(\underline{\hat S}^{(1)})^2) = (1/2)[s(s+1) - (3/2)]<br />

remember

S_{1}^{2} = S_{2}^{2} = (1/2)[(1/2) + 1]
 
But what if we have u_{\frac{1}{2}}^1u_{-\frac{1}{2}}^2

How do we calculate \underline{\hat S}^2u_{\frac{1}{2}}^1u_{-\frac{1}{2}}^2 ?
 
[QUOTE said:
dreamspy;2493358]But what if we have u_{\frac{1}{2}}^1u_{-\frac{1}{2}}^2

How do we calculate \underline{\hat S}^2u_{\frac{1}{2}}^1u_{-\frac{1}{2}}^2 ?
[/QUOTE]

That is a singlet state which has s = 0.
 

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