Hermitian operators and cummutators problem

nakbuchi
Messages
2
Reaction score
0
A,B and C are three hermitian operators such that [A,B]=0, [B,C]=0.
Does A necessarily commutes with C?
 
Physics news on Phys.org


yes since if [A,B] \psi = 0 , [B,C] \psi = 0 that means that there exists a psi which is an eigenstate of all three and all operators commute

or you could try the Jacobi identity
 


@sgd37:
A and B have some common eigenvectors, and so does B and C; but it doesn't necessarily mean that A and C will have common eigenvectors.
 
Last edited:


Sure. But in that case you have some kind of algebra going on. I was naive in thinking they belonged to the same set. But no. If you consider the components of the angular momentum operator and the L^2 operator
 
Last edited:


No, from the Jacobi identity one obtains

[[C,A],B] = 0
 


No, let A = x, B = y, C = px

[A, B] = [x, y] = 0

[B, C] = [y, px] = 0

But,

[A, C] = [x, px] = i \hbar \neq 0
 
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