Do Lz and L^2 Commute?

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Homework Help Overview

The discussion revolves around the commutation of the operators Lz and L^2 in quantum mechanics, specifically focusing on their definitions and implications in the context of wavefunctions.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the definitions of Lz and L^2, questioning how to demonstrate their commutation. Some express uncertainty about the application of the product rule in differentiation involving these operators.

Discussion Status

There is ongoing exploration of the properties of the operators, with some participants attempting calculations and others questioning the assumptions made in their approaches. Guidance has been offered regarding the treatment of constants in differentiation and the use of the product rule.

Contextual Notes

Participants note the complexity of the operators involved and the potential need for assumptions about the continuity of wavefunctions and their derivatives. There is also mention of the independence of the variables theta and phi in the differentiation process.

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Homework Statement


Using the definitions of Lz and L^2, show that these two operators commute.


Homework Equations


Lz = -ih_bar * d/d(phi)
L^2 = -(h_bar)^2 {1/sin(theta) * d/d(theta) * [sin(theta) * d/d(theta)] + 1/sin^2(theta) d^2/d(phi)^2}


The Attempt at a Solution


I'm actually not too sure how to begin this. If someone can show me an example of commuting operators that is a bit complex, that would definitely help. My professor only gave us a simple example, which is why I'm confused with this one. Thanks for your help!
 
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If [itex][L^2,L_z]=0[/itex] (that is L^2 and L_z commute), what can you say about [itex]L^2(L_z\psi)[/itex] and [itex]L_z(L^2\psi)[/itex] for any wavefunction [itex]\psi[/itex]?
 
[tex]x\partial_x[/tex] and [tex]y\partial_y[/tex] commute because
[tex]x\partial_x ( y\partial_y ( f) ) = y\partial_y ( x\partial_x (f))[/tex] for any function f.

On the other hand, [tex]x\partial_y[/tex] does not commute with [tex]y\partial_x[/tex]
 
gabba, I would say that LaTeX Code: L^2(L_z\\psi) and LaTeX Code: L_z(L^2\\psi) for any wavefunction LaTeX Code: \\psi would be equivalent.

My problem is more with doing the problem. Do I do the product rule when it comes to -h_bar^2 * 1/sin(theta) * d/d(theta), or is -h_bar^2 pulled out to the front and I just take the derivative of 1/sin(theta)?
 
Well, -h_bar^2 is a constant isn't it...don't you always pull the constants out when taking a derivative?

Why don't you post an attempt and I'll see where you might be going wrong...
 
constants shouldn't matter in differentiation and keep in mind a phi partial derivative means theta is kept constant for the dervative

might help to remember that the partial derivative cross terms are the same for continuous & differentiable functions ie

for f(u,v) then fuv = fvu

(what are the exact conditions for this to apply?)

So maybe make some assumtions about the wavefunction continuity & its derivatives etc...
 
this is what i have...
Lz(L^2) = ih_bar^3 * {[1/cos(theta) (sin(theta)) + (cos(theta))*1/sin(theta)] + 1/sin^2(theta)}
simplified...ih_bar^3 [sin(theta)/cos(theta) + cos(theta)/sin(theta) + 1/sin^2(theta)]

I did the exact same thing for L^2(Lz), but I realize that making a mistake for each of these will result in the same answer.
 
vballpro said:
this is what i have...
Lz(L^2) = ih_bar^3 * {[1/cos(theta) (sin(theta)) + (cos(theta))*1/sin(theta)] + 1/sin^2(theta)}
simplified...ih_bar^3 [sin(theta)/cos(theta) + cos(theta)/sin(theta) + 1/sin^2(theta)]

This makes no sense :confused:

[itex]L_z[/itex] and [itex]L^2[/itex] are differential operators, so their product should be as well. You should have [tex]\frac{\partial^2}{\partial \phi \partial \theta}[/tex] terms in your expression for [itex]L_z(L^2)[/itex].
 
how do i work with 1/sin(theta)d/d(theta) * (sin(theta)d/d(theta)) part?
 
  • #10
do you use the product rule or are they two totally different derivations?
 
  • #11
Use the product rule!

For example,

[tex]\frac{\partial}{\partial x}\left[f(y)\frac{\partial}{\partial y}\left(g(y)\frac{\partial}{\partial y}\right)\right]=\frac{\partial}{\partial x}\left[f(y)g'(y)\frac{\partial}{\partial y}+f(y)g(y)\frac{\partial^2}{\partial y^2}\right]=f(y)g'(y)\frac{\partial^2}{\partial x \partial y}+f(y)g(y)\frac{\partial^3}{\partial x \partial y^2}[/tex]
 
  • #12
2nd time's a charm?
-i*(h_bar)^3 [ cos(theta)/sin(theta) * d^2/d(theta)^2 + d^3/d(theta)^3 + 1/sin^2(theta) * d^3/d^3(theta)

why is it that it's d/dx [ f(y)g'(y) d/dy + f(y)g(y)d^2/dy^2] instead of
d/dx [ f(y)g'(y) d/dy + f'(y)g(y)d^2/dy^2]? (i added in an f ' to the second part. it might be hard to tell with this font.) i thought you said product rule. could you explain?
 
  • #13
vballpro said:
2nd time's a charm?
-i*(h_bar)^3 [ cos(theta)/sin(theta) * d^2/d(theta)^2 + d^3/d(theta)^3 + 1/sin^2(theta) * d^3/d^3(theta)

why is it that it's d/dx [ f(y)g'(y) d/dy + f(y)g(y)d^2/dy^2] instead of
d/dx [ f(y)g'(y) d/dy + f'(y)g(y)d^2/dy^2]? (i added in an f ' to the second part. it might be hard to tell with this font.) i thought you said product rule. could you explain?

Because d/dy acts only on the product g(y) d/dy...it doesn't act on f(y)-which comes before the operator.

And 2nd time is definitely not the charm...sorry::frown:...theta and phi are independent variables...but all I see is theta derivatives in your expression...what happened to the phi derivatives?
 

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