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whose roots (eigenvalues, left in the top row of Figure 7.2) are x ¼ 1,
while the normalized eigenvectors (the MOs of the top row of Figure 7.3)
are given by the (2 2) unitary matrix
0
@
1
A
1
2
1
p
p
C ¼ð c 1 c 2 Þ¼
ð 7
:
55 Þ
1
2
1
2
p
p
7.4.2 The Allyl Radical (N ¼ 3)
uckel secular equation for N ¼ 3is
The H
x 10
1 x 1
01 x
¼ x ð x 2
1 Þþ x ¼ x ð x 2
D 3 ¼
2 Þ¼ 0
ð 7
:
56 Þ
+
-
+
N = 2
+
.
.
.
+
-
-
-
φ 1
φ 2
N = 3
+
.
-
.
+
+
+
+
-
+
.
-
-
-
-
-
+
-
+
φ 1
φ 2
φ 3
N = 4
+
.
+
.
+
.
-
.
+
+
+
-
-
-
-
+
-
-
-
+
φ 1
φ 2
+
+
-
+
-
-
+
-
.
.
.
.
.
.
.
+
+
-
+
-
-
+
-
φ 3
φ 4
Figure 7.3 H
uckel MOs for a linear chain with N ¼ 2
;
3
;
4
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