Diagonalizing a matrix using perturbation theory.

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The discussion revolves around diagonalizing a Hamiltonian matrix using perturbation theory, specifically focusing on the given matrix H and its unperturbed counterpart Ho. Participants express confusion about calculating corrections and the need for wavefunctions, clarifying that eigenstates of the unperturbed Hamiltonian are sufficient for the process. The matrix elements can be derived from the given Hamiltonian representation, which aids in the diagonalization. The conversation emphasizes understanding the relationship between the Hamiltonian and its eigenstates rather than requiring a physical system or wavefunction. Overall, the key takeaway is the importance of identifying the correct eigenstates to facilitate the diagonalization process.
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Homework Statement



Consider the following Hamiltonian.

H=\begin{pmatrix} 20 &amp; 1 &amp; 0 \\1 &amp; 20 &amp; 2 \\0 &amp; 2 &amp; 30 \end{pmatrix}<br />
Diagonalize this matrix using perturbation theory. Obtain eigenvectors (to first order) and eigenvalues (to second order).

Ho=\begin{pmatrix} 20 &amp; 0 &amp; 0 \\0 &amp; 20 &amp; 0 \\0 &amp; 0 &amp; 30 \end{pmatrix}<br />
H'=\begin{pmatrix} 0 &amp; 1 &amp; 0 \\1 &amp; 0 &amp; 2 \\0 &amp; 2 &amp; 0 \end{pmatrix}<br />

Homework Equations


The Attempt at a Solution



In general, diagonalizing a matrix involves finding its eigenvalues and then writing the eigenvalues on the diagonal with zeros elsewhere. Despite that, I'm just not sure how to approach this question.
 
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How do you calculate corrections in perturbation theory? What equations do you have? Do you have degenerate states?

It's really just a matter of figuring out which formulas you need to use and plugging everything in. You can get the needed matrix elements by inspection.
 
That's what's throwing me off. There is no "physical system" as I have come to understand it. All I'm given is what I wrote above. I understand that to calculate perturbations in general, you use <Psi|H'|Psi>, but that gets me back to needing a wavefunction to operate on. All I have is this set of matrices.
 
You don't need a wave function for the system. You need the eigenstates of the unperturbed Hamiltonian. Let's call those \vert 1 \rangle, \vert 2 \rangle, and \vert 3 \rangle. The matrix you've been given is the representation of \hat{H} relative to that basis. In other words,
\begin{pmatrix}<br /> \langle 1 \lvert \hat{H} \rvert 1 \rangle &amp; \langle 1 \lvert \hat{H} \rvert 2 \rangle &amp; \langle 1 \lvert \hat{H} \rvert 3 \rangle \\<br /> \langle 2 \lvert \hat{H} \rvert 1 \rangle &amp; \langle 2 \lvert \hat{H} \rvert 2 \rangle &amp; \langle 2 \lvert \hat{H} \rvert 3 \rangle \\<br /> \langle 3 \lvert \hat{H} \rvert 1 \rangle &amp; \langle 3 \lvert \hat{H} \rvert 2 \rangle &amp; \langle 3 \lvert \hat{H} \rvert 3 \rangle<br /> \end{pmatrix} = \begin{pmatrix} 20 &amp; 1 &amp; 0 \\1 &amp; 20 &amp; 2 \\0 &amp; 2 &amp; 30 \end{pmatrix}<br />
Does that clear things up?
 
How does that help diagonalize H?
 
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