19.6 Complex matrices 551
or, in terms of components,
l
x
1 = 1 I
xx
ω
x
1 + 1 I
xy
ω
y
1 + 1 I
xz
ω
z
l
y
1 = 1 I
yx
ω
x
1 + 1 I
yy
ω
y
1 + 1 I
yz
ω
z
(19.47)
l
z
1 = 1 I
zx
ω
x
1 + 1 I
zy
ω
y
1 + 1 I
zz
ω
z
When the coordinate axes coincide with the principal axes of inertia, Iis diagonal and
equations (19.47) reduce to
l
x
1 = 1 I
xx
ω
x
, l
y
1 = 1 I
yy
ω
y
, l
z
1 = 1 I
zz
ω
z
(19.48)
The kinetic energy of rotation then has the familiar form
(19.49)
that is used in theoretical discussions of the microwave spectroscopy of polyatomic
molecules.
0 Exercise 35
19.6 Complex matrices
Much of the earlier discussion applies equally well to complex matrices as to real
matrices and, in this section, we summarize the more important properties of complex
matrices, and the ways in which these differ from those of real matrices.
A matrix Awhose elements are complex numbers is called a complex matrix, and
can be written in the form
A 1 = 1 B 1 + 1 iC (19.50)
where , and Band Care real matrices.
The complex conjugate matrix A*
The complex conjugate matrixA*is obtained from Aby replacing each element of
Aby its complex conjugate:
if A 1 = 1 (a
ij
)thenA* 1 = 1 (a
ij
*) (19.51)
and
A* 1 = 1 B 1 − 1 iC (19.52)
For a realmatrix,A* 1 = 1 AandC 1 = 10.
i=− 1
T
l
I
l
I
l
I
x
xx
y
yy
z
zz
=++
2
2
2
222