Any quick help with rearranging schrodinger equation in dirac notation

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The discussion focuses on rearranging the Schrödinger equation in Dirac notation, particularly in the context of relativistic corrections and perturbation theory applied to hydrogen. The user expresses confusion regarding the treatment of the Coulomb potential, specifically the sign of the potential when moved across the equation. It is established that the Coulomb potential, represented as V(r) = e²/(4πε₀r), is indeed a repulsive potential, and the user suggests a possible typo in the initial substitution that should include a negative sign for an attractive potential.

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I'm looking through my lecture notes, (studying relativistic corrections/perturbation theory using hydrogen), and I seem to have a mind block with one of the equations (the last one from the 3 in the middle).

I know that the kinetic energy and coulomb potential has been subbed in for the operator H0, but I don't understand the rearrangement. Simply multiply both sides by 2*m, then take the coulomb potential to the other side.

The coulomb potential (the e^2 term) on the left hand side is positive, moving it to the right would make it negative, so why is it positive?
 

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I know that the kinetic energy and coulomb potential has been subbed in for the operator H0, but I don't understand the rearrangement. Simply multiply both sides by 2*m, then take the coulomb potential to the other side.
... I think I see what you mean.
##V(r)=e^2/4\pi\epsilon_0r## would be a repulsive potential wouldn't it?
If the potential is supposed to be attractive, then they've made a typo in the initial substitution: there should be a minus sign in there.
 

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