Do the Hamiltonian and Angular Momentum Commute in Spherical Coordinates?

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Homework Help Overview

The discussion revolves around the commutation relationship between the Hamiltonian and the z-component of angular momentum in the context of quantum mechanics, specifically in spherical coordinates. The original poster presents the Hamiltonian and angular momentum operators and seeks to understand their commutation properties.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Participants explore the commutation relation by considering the definitions of the Hamiltonian and angular momentum operators. Some suggest using the Laplace operator in spherical coordinates and the properties of derivatives. Others raise questions about the dependence of the potential on the angular variable and its implications for commutation.

Discussion Status

The discussion is ongoing, with participants providing hints and suggestions for approaching the problem. Some guidance has been offered regarding the use of test functions and the application of the Laplacian in spherical coordinates. Multiple interpretations of the problem are being explored, particularly concerning the dependence of various terms on the angular variable.

Contextual Notes

Participants note that if the potential is a function of the angular variable, the Hamiltonian may not commute with the angular momentum operator. There is also mention of the need to clarify the role of test functions in the context of operator commutation.

eit32
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Do the Hamiltonian (H) and the z-component of angular momentum (L_z) commute?
[H, L_z]=0

H = [(-(hbar)^2/2m) dell^2] + V(r, theta, phi)
where dell is the gradient, and V is the potential

L_z = -i(hbar)(d/d phi)
where d is actually a partial derivative

I know how to find a commutator : [H,L_Z] = H*L_z - L_z*H
but I'm having trouble working through it in spherical coordinates (which my problem calls for)
 
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Take a math handbook and look for Laplace operator in spherical coordinates. Then use the rule that derivative with recpect to fi commutes with derivatives with respect to other variables.
 
If V is a function of phi, H won't commute with L_z.
 
it depends on what kind of H you have.


When one have operators that contais derivatives, one usally let's the commutatur act on a test function, i.e :

[A,B]\psi(\vec{x}) = A(B\psi(\vec{x}))-B(A\psi(\vec{x}))
 
I have been using a test function but everything keeps canceling out and i don't think its suppose to
 
just use a general test function, denote it \psi(r, \phi, \theta)

Show how you did, and use Lojzek's hint to use the laplacian in spherical coordinates
 
1. On what single spherical coordinate variable does Lz depend?

2.Does the KE depend on this variable?

3. Can a potential depend on this variable?There is no need to use a test function; you are dealing with operators in the same fashion as with the commutator of p and q.

Regards,
Reilly Atkinson
 
so:

HL_z \approx H\frac{\partial}{\partial \phi}

what is the derivative operator acting on if you don't have a test function?
 

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