Acceleration operator and the electron in a hydrogen atom

[QuasiParticle]

I am wondering about acceleration in quantum mechanics. Let's consider spherically symmetric potential V(r). From the Heisenberg equation of motion, one finds the time derivative of the momentum operator

\dot{\hat{p}}=\frac{i}{\hbar}\left[\hat{H},\hat{p}\right] = -\nabla V,
from which we can construct an acceleration operator simply by

\hat{a} = -\frac{1}{m} \nabla V .
I then want to apply this to the electron in a hydrogen atom. The expectation value of the acceleration is undoubtedly zero for every state. But the RMS-value could be expected to be non-zero. The calculation of the expectation value

\langle \Psi_{nlm} | \hat{a}^2 | \Psi_{nlm} \rangle
for the ground state

\Psi_{100}(r,\theta,\phi)=\frac{1}{\sqrt{\pi a_0^3}}e^{-r/a_0}
gives a divergent result due to the Coulomb potential. The same evidently happens with all other states of hydrogen as well. I don't know how to interpret this result. Is acceleration not a good observable in quantum mechanics?

 

[mfb]

You should get a finite value if you take into account that the proton radius is finite. That does not help for positronium, of course.
Alternatively, you could consider <|a|>.

 

[QuasiParticle]

Thanks mfb!

You should get a finite value if you take into account that the proton radius is finite. That does not help for positronium, of course.

I thought about assigning the problem to the Coulomb potential, but as you say, it does not save the case of a "point nucleus" (e.g. positronium).

Alternatively, you could consider <|a|>.

You are right, \langle |\hat{a}| \rangle gives a finite value. But it seems strange that the RMS expectation cannot be calculated. I wonder if this reflects some deeper property of the "acceleration operator", or just misuse of the Coulomb potential in ordinary QM, etc.

 

[The_Duck]

You would have the same problem if, say, you wanted to calculate the expectation value of 1/|x| for the 1D harmonic oscillator ground state. The expectation value really is infinite. I don't think this indicates any sort of pathology (it does suggest that in practice no apparatus can really measure the quantity 1/|x|, which is sensible: any real apparatus will have a finite position resolution which will cut off the divergent integral).

 

[HomogenousCow]

Is there some other way to differentiate an operator?