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is the nuclear magneton and g N ¼ 5
585. Connected to the nuclear spin
equivalent of (5.13) is the nuclear magnetic resonance (NMR), an experi-
mental technique of great importance nowadays in structural organic
chemistry.
:
5.2 THE PAULI EQUATIONS FOR
ONE-ELECTRON SPIN
Until now nothing has been said about the x and y components of the
vector operator S . If we introduce the spin ladder operators
S þ ¼ S x þ iS y ;
S ¼ S x iS y
ð 5
:
15 Þ
(i being the imaginary unit, i 2
¼ 1), 3 then the analogy with orbital
angular momentum suggests for spin the two-step ladder of Figure 5.1,
where the operators S þ and S respectively step-up (raise) or step-down
(lower) the spin functions upon which they act. Therefore, it is intuitive
that
(
S þ a ¼ 0 ð top of the ladder Þ;
S a ¼ b
ð 5
:
16 Þ
S þ b ¼ a;
S b ¼ 0 ð bottom of the ladder Þ
By adding and subtracting the corresponding equations, it is easily seen
that the two spin states
a
and
b
do satisfy the equations
<
1
2 b;
1
2 i
1
2 a
S x a ¼
S y a ¼
S z a ¼
b;
ð 5
:
17 Þ
1
2 a;
1
2 i
1
2 b
:
S x b ¼
S y b ¼
S z b ¼
a;
which are known as Pauli's equations for the one-electron spin and which
are of fundamental importance for thewhole theory of spin, even inmany-
electron systems.
Since
2
2
x þ S
2
y þ S
2
z
S
¼ S S ¼ S
ð 5
:
18 Þ
S þ and S have the commutation properties ½ S z ; S þ ¼ S þ ; ½ S z ; S ¼ S ; ½ S 2
; S ¼ 0.
3
 
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