Hi, just wondering whether the commutation relation [\phi,L_3]=i\hbar holds and similar uncertainty relation such as involving X and Px can be derived ?
thanks
Homework Statement
Prove:
[σ⋅(p-qA)]²=(p-qA)²-q\bar{h}σ⋅B
where B=∇×A , p=i\bar{h}∇ and q is constant
Homework Equations
The Attempt at a Solution
if the x component is: px-qAx
and the y component is py-qAy
Then the x and y components shouldn't commute [px-qAx,py-qAy]...
In reviewing the derivation of the quantization of angular momentum-like operators from their commutation relations, I noticed that there is nothing a priori from which you can deduce the degeneracy of the eigenstates. While this is not a problem for angular momentum, in which other constraints...
Let the translation operator be:
F (\textbf {l} ) = exp \left( \frac{-i \textbf{p} \cdot \textbf{l}}{\hbar} \right)
where p is the momentum operator and l is some finite spatial displacement
I need to find [x_i , F (\textbf {l} )]
let me start with a fundamental commutation relation...
i need to find the commutation relation for:
[x_i , p_i ^n p_j^m p_k^l]
I could apply a test function g(x,y,z) to this and get:
=x_i p_i ^n p_j^m p_k^l g - p_i ^n p_j^m p_k^l x_i g
but from here I'm not sure where to go. any help would be appreciated.
what is it? i need to know everything about it. i know it encompasses a lot of different stuff but yea if someone could point me to a book or webpage that explains it thoroughly.
additionally what does this equal
\sigma_{\mu}\sigma_{\alpha}\sigma_{\alpha}\sigma_{\mu}
those are pauli...
Homework Statement
I need to show the commutation between the spin operator and a uniform magnetic field will produce the same result as the cross product between them.
Does this make sense? I don't see how it can be possible.
Homework Equations
[s,B]
(The s should also have a hat...
Is there a book that explain in a formal way the deduction of symmetry/antisymmetry of bosonic/fermionic wave equation e/o commutation relation? I've often noticed that some people use examples for the introcution, but is there an axiomatic deduction?
Homework Statement
I've just initiated a self-study on quantum mechanics and am in need of a little help.
The position and momentum operators do not commute. According to my book which attemps to demonstrate this property,
(1) \hat{p} \hat{x} \psi = \hat{p} x \psi = -i \hbar...
Homework Statement
The canonical commutation relations for a particl moving in 3D are
[\hat{x},\hat{p_{x}}]= i\hbar
[\hat{y},\hat{p_{y}}]= i\hbar
[\hat{z},\hat{p_{z}}]= i\hbar
and all other commutators involving x, px, y ,py, z , pz (they should all have a hat on eahc of them signifying...
I am working on a problem for homework and am supposed to show that the angular momentum operator squared commutes with H and that angular momentum and H also commute. This must be done in spherical coordinates and everything I see says "it's straightforward" but I don't see it. At least not...
I am reading the first chapter of Sakurai's Modern QM and from pages 30 and 32 respectively, I understand that
(i) If [A,B]=0, then they share the same set of eigenstates.
(ii) Conversely, if two operators have the same eigenstates, then they commute.
But we know that [L^2,L_z]=0...
Hi there, I need a help on one of the commutation proof,
the question is, show that [Lx,L^2]=0 cyclic where L=l1+l2
The expression simplifies to [Lx,l1l2]+[Lx,l2l1] but I'm not sure if they are 0.
Thanks for your help :D
I'm following a derivation (p85 of Symmetry Principles in Quantum Physics by Fonda & Ghirardi, for anyone who has it) in which the following assertion is made:
"...we have
\left[\mathcal{G}_p,\mathbf{r}_i\right] &=& \mathbf{v}_0t\mathcal{G}_p,
\left[\mathcal{G}_r,\mathbf{p}_i\right] &=&...
Hi, I have a question,
As it is said in QM, if two operators commute, they have so many common eigenstates that they form a basis. And the inverse is right.
Now there is the question,
if A,B,C are operators, [A,B]=0, [A,C]=0,
then is "[B,C]=0" also right?
If we simply say A and B, A and C...