Define
(1.1)
The Hydrogen wave function separates into
(1.2)
The last term is
(1.3)
The middle term is
The P in (1.4) is the associated Legendre function. Press[2] gives a short stable code for calculating these. He also gives a warning that "most of the recurrences involving m are unstable, and so dangerous for numerical work. AssoLeg.htm .doc
(1.5)
The associated Laguerre polynomial is
There appear to be no warnings about this function.
(1.6) equation 1.6
(1.7) equation 1.7
(1.8)
The
ground state H wave function in the limit as r infinity is
The 2s Li wave function in the limit as r infinity is
The 3s Na wave function in the limit as r infinity is
In each case the Zeff is on the order of 1, owing to the fact that the inner shells are filled. Note that the higher order states are beginning to have a constant wave function in the asymptotic regions.
In the K shell region Zeff = 11. In the L shell region Zeff=9. In the M shell region Zeff = 1.

Figure 1 Regions for various Zeff's
The code for plotting the probabilities is for\plotsorbs.for.

Figure 2 The K and L shell of sodium. The M shell is a flat blue at the bottom of the plot.

Figure 3 Scale in y a factor of 12 larger and that in x a factor of 10 larger than in the above figure.
The orbital energy of the 1s state is
(1.9)
This consists of three parts. The probability distribution
(1.10)
This is prepared for plotting on an even grid in for\plotsorbs.for. The potential energy distribution
(1.11)
And finally. the Kinetic energy distribution is given by
(1.12)
Remember that the Zeff is crude, define the
derivative to be
Approximate to handle the negative value at the
origin. Use the Zeff’s of
figure 1. E.g.
Use the BLI to find P(r), V(r), and T(r). Plot these and send me the plots.