Commutation and Eigenfunctions

CanIExplore
Messages
97
Reaction score
0
My first question is, does any operator commute with itself? If this is the case, is there a simple proof to show so? If not, what would be a counter-example or a "counter-proof"?

My second question has to do with the properties of an eigenvalue problem. If you have an operator Q such that \hat{Q}\psi=\lambda\psi, then is the following always true?

\hat{Q}^{2}\psi=\lambda^{2}\psi

Since \hat{Q}^{2}\psi=\hat{Q}\hat{Q}\psi=\hat{Q}\lambda\psi=\lambda\hat{Q}\psi=\lambda\lambda\psi=\lambda^{2}\psi.

And is there a more general way of saying this? Like,

\hat{Q}_{i}\hat{Q}_{j}\psi=\hat{Q}_{i}\lambda_{j}\psi=\lambda_{j}\hat{Q}_{i}\psi=\lambda_{i}\lambda_{j}\psi

Which should always be true even if the operators don't commute because the lambdas are just scalars right?
 
Last edited:
Physics news on Phys.org


Of course an operator commutes with itself [Q,Q] is always 0 from the definition of the commutator

For the last part you wouldn't be able to write it like that if the operators don't commute. Commuting operators have simultaneous eigenfunctions, non-commuting ones do not
 
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