18.3 Matrix algebra 511
where and A1= 1 h 22 π where his Planck’s constant. The commutation
properties of these matrices are
[S
x, S
y] 1 = 1 S
xS
y1 − 1 S
yS
xand similarly for the other pairs. Therefore
[S
x, S
y] 1 = 1 iAS
z,[S
y, S
z] 1 = 1 iAS
x,[S
z, S
x] 1 = 1 iAS
y(18.34)
In addition,
and similarly forS
y2andS
z2. Therefore
(18.35)
represents the square of spin angular momentum. The quantity is the square of
the magnitude of the spin angular momentum of an electron, whose (total) spin
quantum number is ,
(18.36)
0 Exercise 42
Multiplication by a unit matrix
If Ais an m 1 × 1 nmatrix and if I
mand I
nare the unit matrices of orders mand n,
respectively, then
I
mA 1 = 1 A 1 = 1 AI
n(18.37)
ss()+=, 1 s=
3
4
1
2
22for
s=
12342SSS I
xyz222 23
4
++=
SSS
xxx22 21
4
01
10
01
10
1
4
1
==
=
00
01
1
4
2
= I
=
−
=
1
2
10
01
2ii
zS
=
−
−
−
1
4
0
0
0
0
2i
i
i
i
=
−
−
−
1
4
01
10
0
0
0
0
2i
i
i
i
01
10
i=− 1 ,