I'm having trouble doing it. I know so far that if we have two Hermitian operators A and B that do not commute, and suppose we wish to find the quantum mechanical Hermitian operator for the product AB, then
AB+BA2.
However, if I have to find an operator equivalent for the radial component of momentum, I am puzzled. It does not come out to be simply
→p⋅→rr+→rr⋅→p2,
where →r and →p are the position and the momentum operator, respectively. Where am I wrong in understanding this?
Answer
You would have to use the fact that the momentum operator in position space is →p=−iℏ→∇ and use the definition of the gradient operator in spherical coordinates:
→∇=ˆr∂∂r+ˆθ1r∂∂θ+ˆϕ1rsinθ∂∂ϕ
So the radial component of momentum is
pr=−iℏˆr∂∂r
However: after a bit of investigation prompted by the comments, I found that in practice this is not used very much. It's more useful to have an operator p′r that satisfies
−ℏ22m∇2R(r)=p′2r2mR(r)
This lets you write the radial component of the time-independent Schrödinger equation as
(p′2r2m+V(r))R(r)=ER(r)
The action of the radial component of the Laplacian in 3D is
∇2R(r)=1r2∂∂r(r2∂R(r)∂r)
and if you solve for the operator p′r that satisfies the definition above, you wind up with
p′r=−iℏ(∂∂r+1r)
This is called the "radial momentum operator." Strictly speaking, it is different from the "radial component of the momentum operator," which is, by definition, pr as I wrote it above, although I wouldn't be surprised to find people mixing up the terminology relatively often.
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