Let us focus on normal matrices. A
matrix
A A is normal if it
commutes with
AH
A
That is,
AAH=AHA
A
A
A
A
(1)
A=010001100
A
0
1
0
0
0
1
1
0
0
AAH
≟
AHA
A
A
≟
A
A
(2)
010001100001100010
≟
001100010010001100
0
1
0
0
0
1
1
0
0
0
0
1
1
0
0
0
1
0
≟
0
0
1
1
0
0
0
1
0
0
1
0
0
0
1
1
0
0
(3)
100010001=100010001
1
0
0
0
1
0
0
0
1
1
0
0
0
1
0
0
0
1
(4)
We will use normal matrices a
lot in ELEC 301
A special case of a normal matrix is a symmetric
matrix where
A=AH
A
A
(5)
ie: row
i
=
i
column
i
i.
- When normalized to
∥vi∥2=1
2
x
v
i
1
, their eigenvectors form an
ONB for
ℂN
N
.
-
They can be diagonalized
A=VΛVH
A
V
Λ
V
(6)
where
Λ Λ is a
diaglonal matrix of eigenvalues
λ
1
0000
λ
2
0000...
...00...
λ
N
-
1
λ
1
0
0
0
0
λ
2
0
0
0
0
...
...
0
0
...
λ
N
-
1
Show that 2 is true using 1.
Avi=λivi
A
v
i
λ
i
v
i
(7)
for
i=0
i
0
,
1
1,
2
2, ...,
N-1
N
1
∥vi∥2=1
2
v
i
1
(8)
V=v0v1v2...v
N
-
1
V
v
0
v
1
v
2
...
v
N
-
1
ONB meatix implies
VHV=I
V
V
I
(9)
VVH=I
V
V
I
(10)
Σ=
λ
1
0000
λ
2
0000...
...00...
λ
N
-
1
Σ
λ
1
0
0
0
0
λ
2
0
0
0
0
...
...
0
0
...
λ
N
-
1
Show that
A=VΛVH
A
V
Λ
V
(11)
AV=VΛVHV
A
V
V
Λ
V
V
(12)
AV=VΛ
A
V
V
Λ
(13)
look in detail at the LHS
AV=Av0v1v2...v
N
-
1
A
V
A
v
0
v
1
v
2
...
v
N
-
1
(14)
AV=Av0Av1Av2...Av
N
-
1
A
V
A
v
0
A
v
1
A
v
2
...
A
v
N
-
1
(15)
why?
AV=λ0v0λ1v1λ2v2...
λ
N
-
1
v
N
-
1
A
V
λ
0
v
0
λ
1
v
1
λ
2
v
2
...
λ
N
-
1
v
N
-
1
(16)
AV=
λ
1
0000
λ
2
0000...
...00...
λ
N
-
1
v0v1v2...v
N
-
1
A
V
λ
1
0
0
0
0
λ
2
0
0
0
0
...
...
0
0
...
λ
N
-
1
v
0
v
1
v
2
...
v
N
-
1
(17)
AV=ΛV
A
V
Λ
V
(18)
=
RHS.
A=3-1-13
A
3
-1
-1
3
since symmetric,
A
A is normal.
From earlier we have
V=v0v1=12111-1
V
v
0
v
1
1
2
1
1
1
-1
Λ=2004
Λ
2
0
0
4
compute
VΛVH
V
Λ
V
=12111-12004111-112
1
2
1
1
1
-1
2
0
0
4
1
1
1
-1
1
2
(19)
=12111-1224-4
1
2
1
1
1
-1
2
2
4
-4
(20)
=126-2-26=3-1-13=A
1
2
6
-2
-2
6
3
-1
-1
3
A
(21)
- Every normal matrix
A A has a
natural basis (ONB) formed by its
eigenvectors.
- We can
diagonalize any normal matrix
A
A by
A=VΛVH
A
V
Λ
V
(22)
Sometimes it is much more efficient to apply
VH
V
then
Λ
Λ then
V
V than
A
A.
-
A Ais completely
characterized by its eigenvectors
vi
v
i
and eigenvalues
λi
λ
i