Commutator problem with momentum operators

Join the discussion
Ask a follow-up here, or get your own question answered by working scientists, mathematicians and engineers — people, not an autocomplete.
Real named experts · corrections over time · the nuance an AI answer skips
8 replies · 3K views
hellomister
Messages
29
Reaction score
0

Homework Statement


Find the commutator [tex] \left[\hat{p_{x}},\hat{p_{y}}\right][/tex]


Homework Equations


[tex]\hat{p_{x}}=\frac{\hbar}{i}\frac{\partial}{\partial x}[/tex]

[tex]\hat{p_{y}}=\frac{\hbar}{i}\frac{\partial}{\partial y}[/tex]


The Attempt at a Solution


[tex][\hat{p}_{x}, \hat{p}_{y}]=\hat{p}_{x}\hat{p}_{y}-\hat{p}_{y}\hat{p}_{x}[/tex]

[tex]=\frac{\hbar}{i}\frac{\partial}{\partial x}\frac{\hbar}{i}\frac{\partial}{\partial y}-\frac{\hbar}{i}\frac{\partial}{\partial y}\frac{\hbar}{i}\frac{\partial}{\partial x}[/tex]

[tex]=(\frac{\hbar}{i})^2\frac{\partial^2}{\partial x\partial y}-(\frac{\hbar}{i})^2\frac{\partial^2}{\partial y\partial x}[/tex]

Is this the correct commutator? I don't know what else I can do to further complete this. Any help is appreciated.
 
Physics news on Phys.org
Okay thanks for the response, i have a similar problem to that of the first that I put up, but I am very confused.

Problem
Show that [tex][\hat{L}_{x},\hat{P}_{y}]=i\hbar\hat{P}_{z}.<br /> (Note: \hat{L}_{x}=y\hat{P}_{z}-z\hat{P}_{y})[/tex]
Televant equations
[tex]\hat{p_{x}}=\frac{\hbar}{i}\frac{\partial}{\partial x}[/tex]

[tex]\hat{p_{y}}=\frac{\hbar}{i}\frac{\partial}{\partial y}[/tex]

[tex]\hat{p_{z}}=\frac{\hbar}{i}\frac{\partial}{\partial z}[/tex]

Attempt
So i started out by just writing out the commutator in the general form:

(1) [tex]\hat{L}_{x}\hat{P}_{y}-\hat{P}_{y}\hat{L}_{x}[/tex]

Then I slowly substituted some equations
(2) [tex](y\hat{P}_{z}-z\hat{P}_{y})\frac{\hbar}{i}\frac{\partial}{\partial y}\psi-\frac{\hbar}{i}\frac{\partial}{\partial y}(y\hat{P}_{z}\psi-z\hat{P}_{y}\psi)[/tex]

(3)[tex](y\frac{\hbar}{i}\frac{\partial}{\partial z}-z\frac{\hbar}{i}\frac{\partial}{\partial y})\frac{\hbar}{i}\frac{\partial}{\partial y}\psi-\frac{\hbar}{i}\frac{\partial}{\partial y}(y\frac{\hbar}{i}\frac{\partial}{\partial z}\psi-z\frac{\hbar}{i}\frac{\partial}{\partial y}\psi)[/tex]

I decided to factor out \frac{\hbar}{i}
[tex](4)(\frac{\hbar}{i})^2(y\frac{\partial}{\partial z}-z\frac{\partial}{\partial y})\frac{\partial \psi}{\partial y}-(\frac{\hbar}{i})^2\frac{\partial}{\partial y}(y\frac{\partial \psi}{\partial z}-z\frac{\partial \psi}{\partial y})[/tex]

Now I'm not sure what to do..
 
Now start expanding the derivatives in the second term using the product rule. Look for cancellations with symmetric partial derivatives like dy*dz vs dz*dy.
 
Last edited:
okay so then i got this

(5) [tex](\frac{\hbar}{i})^2(y\frac{\partial}{\partial z}\frac{\partial\psi}{\partial y}-z\frac{\partial}{\partial y}\frac{\partial\psi}{\partial y})-(\frac{\hbar}{i})^2(\frac{\partial\psi}{\partial z}+y\frac{\partial}{\partial y}\frac{\partial\psi}{\partial z}-\frac{\partial z}{\partial y}\frac{\partial\psi}{\partial y}+z\frac{\partial}{\partial y}\frac{\partial\psi}{\partial y})[/tex]

So then would [tex]y\frac{\partial}{\partial z}\frac{\partial\psi}{\partial y} y\frac{\partial}{\partial y}\frac{\partial\psi}{\partial z}[/tex] cancel out? I'm not sure what you mean by cancel out haha, i have a really bad math foundation if you could please explain that would help a lot. Also did i do that last line correctly?

[tex]z\frac{\partial}{\partial y}\frac{\partial\psi}{\partial y}[/tex] This term would also go away right?

Thanks for all your help!
 
hellomister said:
okay so then i got this

(5) [tex](\frac{\hbar}{i})^2(y\frac{\partial}{\partial z}\frac{\partial\psi}{\partial y}-z\frac{\partial}{\partial y}\frac{\partial\psi}{\partial y})-(\frac{\hbar}{i})^2(\frac{\partial\psi}{\partial z}+y\frac{\partial}{\partial y}\frac{\partial\psi}{\partial z}-\frac{\partial z}{\partial y}\frac{\partial\psi}{\partial y}+z\frac{\partial}{\partial y}\frac{\partial\psi}{\partial y})[/tex]

So then would [tex]y\frac{\partial}{\partial z}\frac{\partial\psi}{\partial y} y\frac{\partial}{\partial y}\frac{\partial\psi}{\partial z}[/tex] cancel out? I'm not sure what you mean by cancel out haha, i have a really bad math foundation if you could please explain that would help a lot. Also did i do that last line correctly?

[tex]z\frac{\partial}{\partial y}\frac{\partial\psi}{\partial y}[/tex] This term would also go away right?

Thanks for all your help!

1- The last term has a wrong sign.
2- By 'canceling out' one means finding a term with exactly the same form of a given term in the equation but with reversed sign so both would disappear. As in x+y-z-x=0, x and -x cancel out each other and the equation reduces to y-z=0.
2- Remember that derivatives have no order in the sense that [tex]\frac{\partial}{\partial x}\frac{\partial f(x,y)}{\partial y} = \frac{\partial}{\partial y}\frac{\partial f(x,y)}{\partial x}[/tex].
4- Now start canceling out terms and I'd recall that the derivative of coordinates wrt each other vanishes.

AB
 
what about the (partial z/ partial y) (partial psi/ partial y)?
What does that become?
 
hellomister said:
what about the (partial z/ partial y) (partial psi/ partial y)?
What does that become?

Didn't you notice my fourth remark?!

AB
 
ahh I see what you mean. Thanks for all the help!