Commutator problem with momentum operators

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Homework Help Overview

The discussion revolves around the commutation relations of momentum operators in quantum mechanics, specifically focusing on the commutators of the momentum operators \(\hat{p_{x}}\) and \(\hat{p_{y}}\), as well as the angular momentum operator \(\hat{L}_{x}\) with the momentum operator \(\hat{P}_{y}\).

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to compute the commutator \([\hat{p_{x}}, \hat{p_{y}}]\) and questions the correctness of their approach. Other participants point out that partial derivatives commute, suggesting a reevaluation of the original poster's calculations.
  • Another participant presents a related problem involving the commutator \([\hat{L}_{x}, \hat{P}_{y}]\) and outlines their steps, expressing confusion about how to proceed with the calculations and the implications of certain terms canceling out.
  • Questions arise regarding the interpretation of terms and the process of cancellation in the context of partial derivatives.

Discussion Status

The discussion is ongoing, with participants providing feedback and guidance on the calculations. There is an exploration of different interpretations of the terms involved, and participants are actively questioning and clarifying their understanding of the mathematical properties of the operators.

Contextual Notes

Participants are working under the constraints of homework assignments, which may limit the information they can access or utilize. There is a focus on ensuring the correct application of mathematical principles related to derivatives and commutation relations.

hellomister
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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.
 
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It's fine. But partial derivatives commute in the physics sense. Your two partial derivatives are equal.
 
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!
 

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