## Degeneracy and diagonalization

Posted by peeterjoot on November 10, 2011

# Motivation.

In class it was mentioned that to deal with perturbation around a degenerate energy eigenvalue, we needed to diagonalize the perturbing Hamiltonian. I didn’t follow those arguments completely, and I’d like to revisit those here.

# A four state Hamiltonian.

Problem set 3, problem 1, was to calculate the energy eigenvalues for the following Hamiltonian

This is more complicated that the two state problem that are solved exactly in section 13.1.1 in the text [1], but differs from the (possibly) infinite dimensional problem that was covered in class. Unfortunately, the solution provided to this problem didn’t provide the illumination I expected, so let’s do it again, calculating the perturbed energy eigenvalues for the degenerate levels, from scratch.

Can we follow the approach used in the text for the two (only) state problem. For the two state problem, it was assumed that the perturbed solution could be expressed as a superposition of the two states that formed the basis for the unperturbed Hilbert space. That is

For the two state problem, assuming that the perturbed energy eigenvalue is , and the unperturbed energy eigenvalue is we find

Left multiplying by the brakets we find

Or

Observe that there was no assumption about the dimensionality of and here, just that the two degenerate energy levels had eigenvalues and a pair of eigenkets and such that . It’s clear that we can use a similar argument for any degeneracy degree. It’s also clear how to proceed, since we have what almost amounts to a characteristic equation for the degenerate subspace of Hilbert space for the problem.

Because is Hermitian, a diagonalization

can be found. To solve for we can take the determinant of the matrix factor of 2.5, and because we have

So our energy eigenvalues associated with the perturbed state are (exactly)

It’s a bit curious seeming that only the energy eigenvalues associated with the degeneracy play any part in this result, but there is some intuitive comfort in this idea. Without the perturbation, we can’t do an energy measurement that would distinguish one or the other of the eigenkets for the degenerate energy level, so it doesn’t seem unreasonable that a perturbed energy level close to the original can be formed by superposition of these two states, and thus the perturbed energy eigenvalue for the new system would then be related to only those degenerate levels.

Observe that in the problem set three problem we had a diagonal initial Hamiltonian , that doesn’t have an impact on the argument above, since that portion of the Hamiltonian only has a diagonal contribution to the result found in 2.5, since the identity removes any requirement to know the specifics of that portion of the matrix element of .

# Generalizing slightly.

Let’s work with a system that has kets using an explicit degeneracy index

**Example:**

Again we seek to find the energy eigenvalues of the new system

For any with associated with a degeneracy () we can calculate the subspace diagonalization

where

and is diagonal

This isn’t a diagonalizing transformation in the usual sense. Putting it together into block matrix form, we can write

and find that a similarity transformation using this change of basis matrix puts all the block matrices along the diagonal into diagonal form, but leaves the rest possibly non-zero

## A five level system with two pairs of degenerate levels.

Let’s do this explicitly using a specific degeneracy example, supposing that we have a non-degenerate ground state, and two pairs doubly degenerate next energy levels. That is

Our change of basis matrix is

We’d like to calculate

Let’s write this putting row and column range subscripts on our matrices to explicitly block them into multiplication compatible sized pieces

The change of basis calculation then becomes

We see that we end up with explicitly diagonal matrices along the diagonal blocks, but products that are otherwise everywhere else.

In the new basis our kets become

Suppose we calculate this change of basis representation for (we’ve implicitly assumed above that our original basis had the ordering ). We find

With

We find

## Energy eigenvalues of the unperturbed Hamiltonian in the new basis.

Generalizing this, it is clear that for a given degeneracy level, the transformed kets in the new basis are superposition of only the kets associated with that degenerate level (and the kets for the non-degenerate levels are left as is).

Even better, we have for all that remain eigenkets of the unperturbed Hamiltonian. We see that by computing the matrix element of our Hamiltonian in the full basis.

Writing

or

where has been shown to have diagonal block diagonals, we can write

So in the basis, our Hamiltonian’s matrix element is

When , application of this Hamiltonian to the new basis kets gives

But this is just

a statement that the are still the energy eigenkets for the unperturbed system. This matches our expectations since we’ve seen that these differ from the original basis elements only for degenerate energy levels, and that these new basis elements are superpositions of only the kets for their respective degeneracy levels.

# References

[1] BR Desai. *Quantum mechanics with basic field theory*. Cambridge University Press, 2009.

## Leave a Reply