One of the most difficult tasks of the many-body problem of atomic physics
from the point of view of numerical calculations is to include the exchange
energy. In calculations of statistical atomic physics this energy is taken
into consideration with the help of a term which is substantially simpler
than the corresponding wave-mechanical expression and is related to the tot
al density rho of the electrons in the atom. The exchange energy density is
gamma(alpha) = (4/3)chi(alpha)rho(1/3). In a previous work it was shown th
at the reduced effective nucleus charges Z(p)/Z determined using the 'self-
consistent field' method disregarding the exchange energy can be described
by a universal function independent of atomic number if the quantity x = r/
mu proportional to the distance r from the nucleus is introduced as indepen
dent variable. In the present work it is shown that, in the same approach a
s above and with the same independent variable, the quantity rho(1/3)/Z(2/3
) can also be described by a universal function. With the use of the densit
y expression obtainable in this way, the statistical exchange potential can
thus be given in a universal form and then applied in wave-mechanical calc
ulations. It is expected that the sum of the exchange potential and the ele
ctrostatic potential proposed in the previous work gives a good approximati
on of the Hartree-Fock potential. Calculations with this potential are made
in order to determine the eigenfunctions and the energies of the electrons
of the free Cu atom. The integration of the one-electron Schrodinger equat
ion is carried out numerically. The results are reported in Tables 2-10, wh
ere, for the ion Cu+, the solutions of the Fock equations are included as w
ell for comparison purposes. From the data of the tables, it appears clearl
y that the eigenfunctions and eigenvalues calculated using the method propo
sed here are in good agreement with the eigenfunctions and energy values de
termined using the Hartee-Fock method. (C) 2000 Elsevier Science B.V. All r
ights reserved.