(a) Use the recursion formula (Equation 4.76) to confirm that when ℓ=n−1 the radial wave function takes the form
Rn(n−1)=Nnrn−1e−r/na,
and determine the normalization constant Nn by direct integration.
(b) Calculate ⟨r⟩ and ⟨r2⟩ for states of the form ψn(n−1)m.
(c) Show that the "uncertainty" in r (σr) is ⟨r⟩/2n+1 for such states. Note that the fractional spread in r decreases, with increasing n (in this sense the system "begins to look classical," with identifiable circular "orbits," for large n). Sketch the radial wave functions for several values of n, to illustrate this point.