Help with vector operator Del.

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Homework Help Overview

The discussion revolves around a problem in quantum mechanics related to the Pauli theory of the electron, specifically involving the expression (p - eA)X(p - eA)ψ, where ψ is a scalar function and A is the magnetic vector potential. Participants are tasked with showing that this expression reduces to ieBψ, with B being the magnetic induction related to A.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • Participants explore the manipulation of the expression involving the momentum operator p and the vector potential A. There is discussion about the non-commutativity of operators and the implications for the expression's simplification. Questions arise regarding specific equalities and the validity of certain assumptions in the context of operator algebra.

Discussion Status

The discussion is ongoing, with participants sharing insights and questioning assumptions. Some have expressed confusion about specific operator relationships and are seeking clarification on their implications for the problem at hand. There is no explicit consensus, but participants are engaging with the material and exploring different lines of reasoning.

Contextual Notes

Participants are grappling with the complexities of operator algebra in quantum mechanics, particularly in relation to the properties of differential operators and functions of position. The discussion reflects the challenges of applying theoretical concepts to specific expressions in the context of the problem.

cesaruelas
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Homework Statement


In the Pauli theory of the electron, one encounters the expresion:

(p - eA)X(p - eA

where ψ is a scalar function, and A is the magnetic vector potential related to the magnetic induction B by B = ∇XA. Given that p = -i∇, show that this expression reduces to ieBψ.

Homework Equations



pXp = 0 and AXA = 0

The Attempt at a Solution



I've come to this:

-e(pXA + AXp

but I don't even have a clue where to go next since, for all I know,

pXA + AXp = -(AXp) + AXp = 0

?

Someone's got a clue what I should do next? Am I missing something here?
 
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cesaruelas said:

Homework Statement


In the Pauli theory of the electron, one encounters the expresion:

(p - eA)X(p - eA

where ψ is a scalar function, and A is the magnetic vector potential related to the magnetic induction B by B = ∇XA. Given that p = -i∇, show that this expression reduces to ieBψ.

Homework Equations



pXp = 0 and AXA = 0

The Attempt at a Solution



I've come to this:

-e(pXA + AXp

but I don't even have a clue where to go next since, for all I know,

pXA + AXp = -(AXp) + AXp = 0

?

Someone's got a clue what I should do next? Am I missing something here?

xp-px isn't 0. That's not zero for the same reason. The vector potential is a function of x. x doesn't commute with the x component of the momentum operator.
 
Dick said:
xp-px isn't 0. That's not zero for the same reason. The vector potential is a function of x. x doesn't commute with the x component of the momentum operator.

Thank you! I got it now. But now I have another question:

Is

pXA = (-AXp + pXA)/2 or -AXp + pXA

I need to use this result to end up the problem but it would only work if the sencod result is true. I used -AXp = pXA to develop it but the 1/2 is not letting me move on with the problem in question.
 
cesaruelas said:
Thank you! I got it now. But now I have another question:

Is

pXA = (-AXp + pXA)/2 or -AXp + pXA

I need to use this result to end up the problem but it would only work if the sencod result is true. I used -AXp = pXA to develop it but the 1/2 is not letting me move on with the problem in question.

Don't know. I don't know why you think either one is true.
 
Dick said:
Don't know. I don't know why you think either one is true.

pXA = -AXppXA = (pXA + pXA)/2 = (-AXp + pXA)/2
 
cesaruelas said:
pXA = -AXppXA = (pXA + pXA)/2 = (-AXp + pXA)/2

But p x A isn't generally equal to -A x p. It's true for constant vectors because the components of constant vectors are constant and they commute. p is a vector of differential operators and A is a vector of functions of position. They don't commute.
 
Dick said:
But p x A isn't generally equal to -A x p. It's true for constant vectors because the components of constant vectors are constant and they commute. p is a vector of differential operators and A is a vector of functions of position. They don't commute.

Maaaaaaan, you're right. I guess I'll have to find another way to solve this then. Thank you!
 

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