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giving
1
1
2
c 1 þ c 1 ¼ 2c 1 ) c 1 ¼
p ;
p
c 2 ¼ 0
;
c 3 ¼ c 1
;
c 2 ¼ 0
;
c 3 ¼
ð 7
:
61 Þ
which is the second column of matrix (7.57).
(c) x 3 ¼
p
<
:
p c 1 þ c 2 ¼ 0
1
:
p c 2 þ c 3 ¼ 0
2
: c 1 þ
p c 3 ¼ 0
c 1 þ c 2 þ c 3 ¼ 1
c 2 þ
ð 7
:
62 Þ
3
:
c 2 ¼
p c 1
1
:
gives now
:
1
3
:
gives
:
c 3 ¼
p c 2 ¼ c 1
so that it is immediately obtained that
p
2
1
2 ;
1
2 ð 7
c 1 þ 2c 1 þ c 1 ¼ 4c 1 ¼ 1 ) c 1 ¼
c 2 ¼
;
c 3 ¼
:
63 Þ
2
which is the third column of matrix (7.57).
It is of interest to evaluate charge and spin density distributions in
the allyl radical, asssuming that the unpaired electron has
a
spin
. It is convenient to write explicitly the three MOs as
1
2
S ¼ M S ¼
p
2
p
2
1
2 ðx 1 þ
1
1
2 ðx 1
f 1 ¼
x 2 þx 3 Þ; f 2 ¼
p ðx 1 x 3 Þ; f 3 ¼
x 2 þx 3 Þ
ð 7
:
64 Þ
r a and
r b components of the
We then have the following for the
distribution function:
1
4 x
2
4 x
1
4 x
2
4 x
2
4 x
3
4 x
2
4 x
3
4 x
r a ¼ f
2
2
2
2
2
2
2
2
2
2
3
1 þf
2 ¼
1 þ
2 þ
3 þ
1 þ
3 ¼
1 þ
2 þ
ð 7
:
65 Þ
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