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(a)
(b)
i
σ g +
σ u +
s 1
s 2
i
σ g +
σ u +
p z 1
-p z 2
(c)
π g
π u
Figure 7.27 The SALCs for s and p states of a diatomic D ∞h molecule. (a) The
σ u +
combinations of s and of p z AOs. (b) The action of the inversion operation for s 1 and p z 1 .(c)
The
σ g + and
π g and
π u degenerate pairs formed from p x and p y orbitals.
Figure 7.28 shows a general MO diagram based on the SALCs we have generated. In
this picture it is assumed that the
-symmetry MOs formed from the s-AOs do not mix
with their counterparts of the same symmetry from p z . This will be the case if the energy
σ
σ u +
6
π g
2
p z
p x
p y
p y
p x
p z
2p
2p
π u
1
σ g +
5
σ u +
4
2s
2s
σ g +
3
Atomic
orbitals
Atomic
orbitals
Figure 7.28 A general MO diagram for diatomic molecules A 2 for second-row elements. This
diagram assumes no hybridization of the
σ g + or
σ u + combinations of s and of p z AOs.
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