Finding normalized eigenfunctions of a linear operator in Matrix QM

Dixanadu
Messages
250
Reaction score
2

Homework Statement


Hey everyone!
The question is this:
Consider a two-state system with normalized energy eigenstates \psi_{1}(x) and \psi_{2}(x), and corresponding energy eigenvalues E_{1} and E_{2} = E_{1}+\Delta E; \Delta E>0

(a) There is another linear operator \hat{S} that acts by swapping the two energy eigenstates: \hat{S}\psi_{1}=\psi_{2} and \hat{S}\psi_{2}=\psi_{1}. Show that the corresponding normalized eigenfunctions of \hat{S} are \phi_{1}(x)=\frac{1}{\sqrt{2}}(\psi_{1}(x)+\psi_{2}(x)) and \phi_{2}(x)=\frac{1}{\sqrt{2}}(\psi_{1}(x)-\psi_{2}(x)), with eigenvalues \lambda_{1}=+1 and \lambda_{2}=-1

Homework Equations


- The regular eigenvalue/eigenvector stuff.
- In matrix mechanics, the wavefunction \psi_{n}(x)=C_{1}(1,0...n)^{T}+C_{2}(0,1,0...n)^{T}+...C_{n}(0...n)^{T}

The Attempt at a Solution


So I've found the matrix associated with the linear operator \hat{S} in the natural basis U_{1}=(1,0)^{T}, U_{2}=(0,1)^{T}; which is:
http://imageshack.com/a/img266/5713/bfo6.jpg
This gives the correct eigenvalues of +1 and -1. But I don't know how to find the eigenfunctions that the question is talking about. I'm not even sure if the matrix is right...
 
Last edited by a moderator:
Physics news on Phys.org
I think the hint I can give is to use that S is linear and consider a linear combination of the 2 vectors psi1 and psi2.
 
But is my matrix correct for S..?
 
Who cares, you needn't use any matrix to solve the problem.
 
what other ways are there that I can solve this? is it the bra-kets? And yea that matrix is wrong, it should be 0 along the diagonal and 1 otherwise. That's the only way it can be linear always and hermitian, which is the requirement.
 
Thread 'Need help understanding this figure on energy levels'
This figure is from "Introduction to Quantum Mechanics" by Griffiths (3rd edition). It is available to download. It is from page 142. I am hoping the usual people on this site will give me a hand understanding what is going on in the figure. After the equation (4.50) it says "It is customary to introduce the principal quantum number, ##n##, which simply orders the allowed energies, starting with 1 for the ground state. (see the figure)" I still don't understand the figure :( Here is...
Thread 'Understanding how to "tack on" the time wiggle factor'
The last problem I posted on QM made it into advanced homework help, that is why I am putting it here. I am sorry for any hassle imposed on the moderators by myself. Part (a) is quite easy. We get $$\sigma_1 = 2\lambda, \mathbf{v}_1 = \begin{pmatrix} 0 \\ 0 \\ 1 \end{pmatrix} \sigma_2 = \lambda, \mathbf{v}_2 = \begin{pmatrix} 1/\sqrt{2} \\ 1/\sqrt{2} \\ 0 \end{pmatrix} \sigma_3 = -\lambda, \mathbf{v}_3 = \begin{pmatrix} 1/\sqrt{2} \\ -1/\sqrt{2} \\ 0 \end{pmatrix} $$ There are two ways...
Back
Top