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27 Canonical Forms 2

The document discusses canonical forms for linear operators on finite-dimensional vector spaces, including diagonal form, triangular form, Jordan canonical form, and rational canonical form. It provides definitions and theorems regarding these forms, examples of computing them, and methods for finding the Jordan canonical form of a matrix. Key topics covered include eigenvalues, eigenvectors, minimal polynomials, nilpotent operators, and chains of vectors.

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Saurav GOYAL
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0% found this document useful (0 votes)
555 views26 pages

27 Canonical Forms 2

The document discusses canonical forms for linear operators on finite-dimensional vector spaces, including diagonal form, triangular form, Jordan canonical form, and rational canonical form. It provides definitions and theorems regarding these forms, examples of computing them, and methods for finding the Jordan canonical form of a matrix. Key topics covered include eigenvalues, eigenvectors, minimal polynomials, nilpotent operators, and chains of vectors.

Uploaded by

Saurav GOYAL
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
Available Formats
Download as PDF, TXT or read online on Scribd
You are on page 1/ 26

Canonical Forms

Michael Freeze
MAT 531: Linear Algebra
UNC Wilmington

Spring 2015

1 / 26
Canonical Forms

I Diagonal Form
I Triangular Form
I Jordan Canonical Form
I Rational Canonical Form

2 / 26
Diagonal Form

Theorem
Let T be a linear operator on a finite-dimensional vector space
V such that the characteristic polynomial of T splits. If the
algebraic and geometric multiplicity of each eigenvalue of T
coincide, then there exists a basis of V for which T has a
diagonal matrix representation.

3 / 26
Triangular Form

Theorem
Let T be a linear operator on a finite-dimensional vector space
V such that the characteristic polynomial of T splits. Then
there exists a basis of V for which T has a triangular matrix
representation.

4 / 26
Invariant Direct-Sum Decompositions
Definition
A vector space V is said to be the direct sum of subspaces
W1 , . . . , Wr when every vector ~v ∈ V can be written uniquely
in the form ~v = w ~1 + w~2 + · · · + w ~ i ∈ Wi for
~ r with w
1 ≤ i ≤ r.
We write V = W1 ⊕ W2 ⊕ · · · ⊕ Wr .
Definition
Let V = W1 ⊕ · · · ⊕ Wr where T (Wi ) ⊆ Wi for 1 ≤ i ≤ r .
We say that T is the direct sum of the Ti when Wi is
T -invariant for 1 ≤ i ≤ r .
Taking Ti = T |Wi to be the restriction of T to Wi for
1 ≤ i ≤ r , we write T = T1 ⊕ · · · ⊕ Tr .

5 / 26
Minimal Polynomial

Definition
Let T be a linear operator on a finite-dimensional vector space
V . A polynomial m(t) is called the minimal polynomial of T
when m(t) is a monic polynomial of least positive degree for
which m(T ) = T0 .

6 / 26
Computation of Minimal Polynomial

Given an n × n matrix A where n is small, we compute powers


of A to obtain I, A, A2 , . . . , An . Form matrix B so that its rows
are the vectorized powers of A. Row reduce the augmented
matrix [B | In+1 ] and identify a dependency among the first p
rows of B where p is minimal.

7 / 26
Example
 
1 0 3
For A =  2 1 1, obtain
−1 0 3
 
1 0 0 0 1 0 0 0 1 1 0 0 0
 1 0 3 2 1 1 −1 0 3 0 1 0 0 
[B | I4 ] = 
 −2
.
0 12 3 1 10 −4 0 6 0 0 1 0 
−14 0 30 −5 1 40 −10 0 6 0 0 0 1

From the reduced row echelon form of [B | I4 ], we obtain


g (t) = 1 − 35 t + 65 t 2 − 16 t 3 as an annihilating polynomial for A.
We obtain m(t) = t 3 − 5t 2 + 10t − 6 is the minimal
polynomial of A.

8 / 26
Primary Decomposition

Theorem
Let T be a linear operator on a finite-dimensional vector space
V with minimal polynomial m(t) = f1 (t)n1 f2 (t)n2 · · · fr (t)nr
where the fi (t) are distinct monic irreducible polynomials.
Then V is the direct sum of the T -invariant subspaces
W1 , . . . , Wr where Wi is the null space of fi (T )ni for
1 ≤ i ≤ r.
Moreover, fi (t)ni is the minimal polynomial of the restriction
of T to Wi .

9 / 26
Nilpotent Operators

Definition
A linear operator T on a finite-dimensional vector space V is
said to be nilpotent when T n = T0 for some positive integer n.
When for some positive integer k we have T k = T0 but
T k−1 6= T0 , we say that k is the index of nilpotency of T .

Definition
A matrix N having 1’s on the superdiagonal and 0’s elsewhere
is said to be a Jordan nilpotent block.
A matrix J(λ) having λ’s on the diagonal, 1’s on the
superdiagonal, and 0’s elsewhere is said to be a Jordan block
belonging to the eigenvalue λ.

10 / 26
Jordan Canonical Form
Theorem
Let T be a linear operator on a finite-dimensional vector space
V whose characteristic and minimal polynomials are,
respectively,

f (t) = (t−λ1 )n1 · · · (t−λr )nr and m(t) = (t−λ1 )m1 · · · (t−λr )mr

where λ1 , . . . , λr are distinct scalars. Then T has a block


diagonal matrix representation in which each diagonal entry is
a Jordan block.

11 / 26
Jordan Canonical Form

f (t) = (t−λ1 )n1 · · · (t−λr )nr and m(t) = (t−λ1 )m1 · · · (t−λr )mr
For each λi , the Jordan blocks belonging to λi have the
following properties:
(i) There is at least one Jordan block belonging to λi of
order mi and all other Jordan blocks belonging to λi are
of order not exceeding mi .
(ii) The sum of the orders of the Jordan blocks belonging to
λi is ni .
(iii) The number of Jordan blocks belonging to λi equals the
geometric multiplicity of λi .
(iv) The number of Jordan blocks of each possible order is
uniquely determined by T .
12 / 26
Example

The following matrix is in Jordan canonical form and has 3


blocks.
 
2 1 0 0 0 0
0 2 0 0 0 0
 
0 0 3 0 0 0
A= 0 0 0

 3 1 0

0 0 0 0 3 1
0 0 0 0 0 3

13 / 26
Chains of Vectors
Consider an n × n Jordan block
 
λ 1 0 ··· 0 0
0 λ 1 0 0
 
0 0 λ 0 0
J =  .. .. ..  .
 
.. ..
. . . . .
 
0 0 0 λ 1
0 0 0 ··· 0 λ
Observe that
(J − λI)~e1 = ~0
(J − λI)~e2 = e~1 =⇒ (J − λI)2 e~2 = ~0
..
.
(J − λI)~ek = e~k−1 =⇒ (J − λI)k e~k = ~0
14 / 26
Example
Consider  
2 1 0 0 0 0
0 2 0 0 0 0
 
0 0 3 0 0 0
A=
0
.
 0 0 3 1 0

0 0 0 0 3 1
0 0 0 0 0 3

15 / 26
Example
Consider  
2 1 0 0 0 0
0 2 0 0 0 0
 
0 0 3 0 0 0
A=
0
.
 0 0 3 1 0

0 0 0 0 3 1
0 0 0 0 0 3
Multiplication by A − 2I:

(A − 2I)~e1 = ~0
(A − 2I)~e2 = e~1

16 / 26
Example
Consider  
2 1 0 0 0 0
0 2 0 0 0 0
 
0 0 3 0 0 0
A= 0
.
 0 0 3 1 0

0 0 0 0 3 1
0 0 0 0 0 3
Multiplication by A − 3I:
(A − 3I)~e3 = ~0

(A − 3I)~e4 = ~0
(A − 3I)~e5 = e~4
(A − 3I)~e6 = e~5

17 / 26
Finding the Jordan Canonical Form of a Matrix

Finding a Jordan basis essentially involves identifying a


number of linearly independent “chains” of vectors
{~v1 , . . . , ~vk } such that

(A − λI)~vj = ~vj−1

for 1 ≤ j ≤ k.

18 / 26
Example :: One Eigenvalue

Find a Jordan canonical form for


 
0 −3 −2
A = 1 3 1 .
1 2 3

19 / 26
Example :: Two Eigenvalues

Find a Jordan canonical form for


 
1 −2 0 0
1 3 1 0
A= 0
.
1 2 1
0 −1 0 1

20 / 26
Example :: Two Eigenvalues

Find a Jordan canonical form for


 
1 0 3 0
1 3 0 3
A= 0
.
0 1 0
0 0 3 1

21 / 26
Example :: One Eigenvalue, Two Blocks

Find a Jordan canonical form for


 
−2 1 −1 −3
−8 3 −4 −8
A=  4 −1
.
3 4
−1 0 −1 0

22 / 26
What does one do when the characteristic
polynomial does not split?

23 / 26
Companion Matrix

Definition
Let p(t) = t k + ak−1 t k−1 + · · · + a1 t + a0 .
The companion matrix of p(t) is the matrix
 
0 0 0 ··· 0 −a0
 1
 0 0 ··· 0 −a1 
 0
 1 0 · · · 0 −a 2

.
· · · · · · · · · · · · · · · ··· 
 
 0 0 0 · · · 0 −ak−2 
0 0 0 · · · 1 −ak−1

24 / 26
Rational Canonical Form

Theorem
Let T be a linear operator on a finite-dimensional vector space
V with minimal polynomial m(t) = f1 (t)m1 f2 (t)m2 · · · fs (t)ms
where f1 (t), . . . , fs (t) are distinct monic irreducible
polynomials.
Then T has a unique block diagonal matrix representation in
which each diagonal entry is a companion matrix.

25 / 26
Example

 
17 −10
Let A = .
29 −17
Find a rational canonical form for A over R.

26 / 26

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