(a) Treat γp2/2μ as a perturbation for the hydrogen-like atom and, using the techniques of Problem 11.16, show that
⟨2μp2⟩n,l,m=2n2μc2Z2α2
(b) Use the results of (a) and Problem 11.16 to show that for the hydrogen atom
⟨K⟩=−21⟨V⟩
in agreement with the virial theorem in quantum mechanics. See Problem 10.13.