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1
r 12
r 1
2
r 2
O
Figure 4.4
The atomic two-electron system
the sumof the two one-electron hydrogenicHamiltonians and the electron
repulsion term (a two-electron operator). This last term hinders separa-
tion of the two-electron Schroedinger eigenvalue equation into two
separate equations, one for each hydrogenic electron. However, approx-
imations are possible through the variation method using the simple
two-electron product variational function:
1
;
2 Þ¼w 1 ð 1 Þw 2 ð 2 Þ
ð 4
:
24 Þ
where the normalized one-electron functions are given by
1
=
2
c 0
p
w 1s ¼
exp ð c 0 r Þ
ð 4
:
25 Þ
Calculation then gives the variational bound
w 1 w 2
1
r 12
w 1 w 2 h 1 þ h 2 þ
¼ 2h 1s1s þð 1s 2
j 1s 2
« w ¼
Þ
ð 4
:
26 Þ
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