Mathematics I
[Canonical Forms]
                                       Dr. Anirban Lakshman
                                        Assistant Professor
                                      Department of Mathematics
                                             IIIT Kalyani
Dr. Anirban Lakshman (IIIT Kalyani)            MAC101             1 / 35
                                      O UTLINE
1    E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
2    M INIMAL P OLYNOMIAL
3    R EFERENCES
Dr. Anirban Lakshman (IIIT Kalyani)     MAC101           2 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
                                             Definition
     Let V be a vector space over the field F and let T be a linear
     operator on V . A Eigen value(or, characteristic value) of T is a
     scalar λ ∈ F such that there is a non-zero vector α ∈ V with
                                      T (α) = λα.
Dr. Anirban Lakshman (IIIT Kalyani)                 MAC101               3 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
                                 Definition of Eigen-vector
     If λ is a eigen value of T , then any non-zero vector α such that
     T (α) = λα is called a Eigen vector of T associated with the
     eigen value λ.
                                  Definition of Eigen-space
     Collection of all α such that T (α) = λα forms a subspace of V .
    This subspace is called the Eigen-space associated with the eigen
    value λ.
       Eigen space is the null space of the linear transformation
       (T − λI).
Dr. Anirban Lakshman (IIIT Kalyani)          MAC101                      4 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
                                          Geometry
                              F IGURE : Eigen Value and Eigen Vector
Dr. Anirban Lakshman (IIIT Kalyani)           MAC101                   5 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
                                      Geometry
     Geometrically, Ax = λx says that under transformation by A,
     eigenvectors experience only changes in magnitude or sign
     but the orientation of Ax in Rn is the same as that of x.
    The eigenvalue λ is simply the amount of stretch or shrink to
     which the eigenvector x is subjected when transformed by A.
     The above depicts the situation in R2
Dr. Anirban Lakshman (IIIT Kalyani)     MAC101                      6 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
                         Definition of Eigen value of a matrix
 If A is an n × n matrix over the F , a eigen value of A in F is a scalar
λ ∈ F such that the matrix A − λI is singular (not invertible).
      The equation Ax = λx can be written in the form
                               (A − λI)x = 0            − (i)
 Thus, λ is an eigenvalue of A if and only if (i) has a non trivial
solution.
 The set of solutions to (i) is N(A − λI), which is a subspace of R n .
The subspace N(A − λI) is called the eigenspace corresponding to
 the eigenvalue λ.
 Any nonzero vector in N(A − λI) is an eigenvector corresponding to
 λ.
Dr. Anirban Lakshman (IIIT Kalyani)            MAC101                     7 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
     Equation (A − λI)x = 0 will have a non trivial solution if and only if
 A − λI is singular or, equivalently, det(A − λI) = 0.           − (ii)
     If the determinant in (ii) is expanded, we obtain an nth-degree
 polynomial in the variable λ:            P(λ) = det(A − λI)
     This polynomial is called the Characteristic Polynomial, and
equation (ii) is called the Characteristic Equation, for the matrix A.
       The roots of the characteristic polynomial are the eigenvalues of
       A.
       An n × n matrix will have n eigenvalues, some of which may be
       repeated.
       A root λ of characteristic polynomial of a matrix A is said to be
       r-fold eigen value of A if the multiplicity of λ is r.
Dr. Anirban Lakshman (IIIT Kalyani)   MAC101                               8 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
T HEOREM
     Let T be a linear operator on a finite-dimensional vector space V
     and let λ be a scalar. Then the followings are equivalent:
(a) λ is a eigen value of T .
(b) The operator (T − λI)is singular (not invertible).
(c) det(T − λI) = 0
Dr. Anirban Lakshman (IIIT Kalyani)   MAC101                             9 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
E XAMPLE
                             
              4 −2             2
     Let A =          and x =
              1 1              1
                                 
                  4 −2 2         6     2
     Since Ax =              =     =3     = 3x.
                  1 1     1      3     1
     So, λ = 3 is an eigenvalue of A and x = (2, 1)T is an eigenvector
     corresponding to λ = 3.
     Actually, any non-zero multiple of x will be an eigenvector, because
                          A(αx) = αA(x) = αλx = λ(αx).
     For example, x = (4, 2)T is also an eigenvector corresponding to
                                      
                 4 −2 4           12        4
     λ = 3.                   =        =3
                 1 1       2       6        2
Dr. Anirban Lakshman (IIIT Kalyani)      MAC101                         10 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
    Example: Find the eigenvalues and the corresponding
                                                                                      3 2
             eigenvectors of the matrix
                                         3 −2
     Solution: The characteristic equation is                             
               3−λ       2
          det                   = 0 =⇒ λ2 − λ − 12 = 0.
                  3   −2 − λ
     Thus, the eigenvalues of A are λ1 = 4 and λ2 = −3.
     Now we find eigen vectors corresponding to λ1 = 4.                                                              
                                                          −1 2
     For this we determine the null space of (A − 4I) =
                                                          3 −6                                           
                                  −1 2       x1     0
     From (A − 4I)x = θ we get                   =
                                  3 −6 x2           0
     Then we get two equations −x1 + 2x2 = 0, 3x1 − 6x2 = 0.
     These two equations are similar.
Dr. Anirban Lakshman (IIIT Kalyani)   MAC101                       11 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
     From these two equations we get x1 = 2x2 .
                                                                                                       T    2x2         2
     So, we get the solution x = (2x2 , x2 ) =         = x2     = x2 (2, 1)T
                                                 x2          1
     Hence, any non zero multiple of (2, 1)T is an eigenvector
     corresponding to λ1 = 4 and {(2, 1)T } is a basis for the eigenspace
     corresponding to λ1 = 4.
     Similarly, to find the eigenvectors for λ2 , we must solve
                                         (A + 3I)x = 0.
     In this case,         {(−1, 3)T }   is a basis for N(A + 3I) and non zero
     multiple of        {(−1, 3)T }   is an eigen vector corresponding to λ2 = −3.
Dr. Anirban Lakshman (IIIT Kalyani)           MAC101                             12 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
    Example: Find the eigenvalues and the corresponding
                                                   
                                             2 −3 1
             eigenvectors of the matrix A = 1 −2 1
                                             1 −3 2
     Solution: The characteristic equation is
                                    
                2−λ      −3       1
          det  1      −2 − λ     1  = 0 ⇒ −λ(λ − 1)2 = 0
                  1      −3     2−λ
     Thus, the eigen values are λ1 = 0, λ2 = λ3 = 1.
     The eigenspace corresponding to λ1 = 0 is N(A − 0I) i.e., N(A),
     which we determine in the usual manner.
                If x = (x1 , x2 , x3 )T ∈ N(A), then Ax = θ   − (i)
Dr. Anirban Lakshman (IIIT Kalyani)       MAC101                       13 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
     From the augmented matrix of A we get,
                                      
       2 −3 1 0               1 0 −1 0
      1 −2 1 0  →  0 1 −1 0 
       1 −3 2 0               0 0 0 0
     So, the system (i) is equivalent to
                          x1 − x3 = 0      − (ii)
                          x2 − x3 = 0      − (iii)
     From (ii) and (iii) we get x1 = x2 = x3
                                                                 
                                                        x1         1
     So, the solution of (i) is x = (x1 , x1 , x1 )T = x1  = x1 1
                                                        x1         1
     Hence, any non zero multiple of (1, 1, 1)T is an eigenvector
     corresponding to λ1 = 0.
Dr. Anirban Lakshman (IIIT Kalyani)     MAC101                          14 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
     Consequently, the eigenspace corresponding to λ1 = 0 consists of
     all vectors of the form α(1, 1, 1)T , where α is a scalar number.
     Now we find the eigenspace corresponding to λ2 = λ3 = 1.
     For this we solve the system (A − I)y = θ;
                                    
                        1 −3 1       y1        0
                 i.e., 1 −3 1 y2  = 0               − (iv )
                        1 −3 1       y3        0
     From the augmented matrix of the system (iv ) we get
                                           
       1 −3 1 0                1 −3 1 0
      1 −3 1 0  →  0 0 0 0 
       1 −3 1 0                0 0 0 0
     So, the system (iv ) is equivalent to x1 − 3x2 + x3 = 0
                                        i.e, x1 = 3x2 − x3
Dr. Anirban Lakshman (IIIT Kalyani)   MAC101                             15 / 35
   E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
     So, the solution of the system of equations (iv ) is
                 x = (x1 , x2 , x3 ) = (3x2 − x3 , x2 , x3 )
                                                    
                                           3            −1
                                     = x2 1 + x3  0 
                                           0             1
     So, the eigen vectors corresponding to λ2 = λ2 = 1 are
     (3, 1, 0), (−1, 0, 1).
     The eigen space corresponding to λ2 = λ3 = 1 is
     L{(3, 1, 0), (−1, 0, 1)}
Dr. Anirban Lakshman (IIIT Kalyani)   MAC101                   16 / 35
                                      O UTLINE
1    E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
2    M INIMAL P OLYNOMIAL
3    R EFERENCES
Dr. Anirban Lakshman (IIIT Kalyani)     MAC101           17 / 35
                                       M INIMAL P OLYNOMIAL
                                      Cayley-Hamilton theorem
T HEOREM
     Every square matrix satisfies its own characteristic equation.
  This theorem states that if A be an n × n matrix and the characteristic
  equation of A be c0 x n + c1 x n−1 + . . . + cn = 0, then
                                 c0 An + c1 An−1 + . . . + cn In = 0.
Dr. Anirban Lakshman (IIIT Kalyani)             MAC101                  18 / 35
                                      M INIMAL P OLYNOMIAL
E XAMPLE
                 
              2 1
     Let A =        Then the characteristic equation of A is
              3 5
                    
         2−x    1
    det                = 0 or, x 2 − 7x + 7 = 0
           3   5−x
     Then by Cayley-Hamilton theorem A2 − 7A + 7I2 = 0
Dr. Anirban Lakshman (IIIT Kalyani)          MAC101            19 / 35
                                       M INIMAL P OLYNOMIAL
                                      Annihilating Polynomials
    Let A be any square matrix. Let J(A) denote the collection of all
  polynomials f (t) for which A is a root of the polynomial f (t),
  i.e., for which f (A) = 0.
  The set J(A) is not empty, because the Cayley-Hamilton theorem
  tells us that the characteristic polynomial of A belongs to J(A).
       If f (t) is an element of J(A), then we say that f (t) annihilates A
       In this case, f (t) is called the Annihilating Polynomials of A.
     A polynomial f (t) ̸= 0 is monic if its leading coefficient equals one.
Dr. Anirban Lakshman (IIIT Kalyani)              MAC101                       20 / 35
                                      M INIMAL P OLYNOMIAL
                           Definition of Minimal Polynomial
     Let A be any square matrix and J(A) denote the collection of all
  polynomials f (t) which annihilates A. Then the monic polynomial of
  lowest degree in J(A) is called the minimal polynomial m(t) of the
  matrix A.
       Minimal Polynomial m(t) of a matrix is unique.
Dr. Anirban Lakshman (IIIT Kalyani)          MAC101                     21 / 35
                                      M INIMAL P OLYNOMIAL
T HEOREM
     The minimal polynomial m(t) of a matrix A divides every polynomial
 which annihilates A. In particular, m(t) divides the characteristic
  polynomial of A.
T HEOREM
     The characteristic polynomial and the minimal polynomial m(t) of a
  matrix A have the same irreducible factors.
T HEOREM
     A scalar λ is an eigenvalue of the matrix A ⇐⇒ λ is a root of the
  minimal polynomial m(t) of A.
Dr. Anirban Lakshman (IIIT Kalyani)          MAC101                      22 / 35
                                      M INIMAL P OLYNOMIAL
                                                     
                                               2 2 −5
Prob: Find the minimal polynomial m(t) of A = 3 7 −15
                                               1 2 −4
=⇒ Characteristic polynomial of A is
                           
       2−t      2      −5
  det  3     7−t     −15  = 0 or, (t − 1)2 (t − 3) = 0.
        1       2    −4 − t
  The minimal polynomial m(t) must divide Characteristic polynomial
  of A. Also, each irreducible factor of Characteristic polynomial
 [ i.e., (t − 1) and (t − 3)] must also be a factor of m(t).
     Thus, m(t) is exactly one of the following:
     f (t) = (t − 1)(t − 3) and g(t) = (t − 1)2 (t − 3).
Dr. Anirban Lakshman (IIIT Kalyani)          MAC101                  23 / 35
                                      M INIMAL P OLYNOMIAL
     Since g(t) is the Characteristic polynomial of A, so g(A) = 0.
  Now we check whether f (t) is satisfies by A or not.
                                                    
                                1 2 −5         −1 2 −5
   f (A) = (A − I)(A − 3I) = 3 6 −15  3 4 −15
                                1 2 −5          1 2 −7
                                              
                                       0 0 0
                                   = 0 0 0
                                       0 0 0
   So, f (t) annihilates A. Also g(t) annihilates A.
     But f (t) is the lowest degree polynomial which annihilates A.
     So, f (t) = (t − 1)(t − 3) is the minimal polynomial of A.
Dr. Anirban Lakshman (IIIT Kalyani)          MAC101                   24 / 35
                                      M INIMAL P OLYNOMIAL
                         Minimal Polynomial of a Linear Operator
    The minimal polynomial m(t)of a linear operator T is defined to be
  the monic polynomial of lowest degree for which T is a root.
  However, for any polynomial f (t), we have f (T ) = 0 ⇐⇒ f (A) = 0,
  where A is any matrix representation of T .
       T and A have the same minimal polynomial.
       The above theorems on the minimal polynomial of a matrix also
       hold for the minimal polynomial of a linear operator.
Dr. Anirban Lakshman (IIIT Kalyani)          MAC101                     25 / 35
                                      D IAGONALISATION
Algebraic multiplicity and Geometric multiplicity of an eigen value
       For an r-fold eigen value λ, r is called the algebraic multiplicity
       (A.M.) of λ.
       Rank of the eigen space corresponding to λ is called the
       Geometric multiplicity (G.M.) of λ.
       1 ≤ Geometric multiplicity ≤ algebraic multiplicity
Definition: An eigen value λ is said to be regular if
     algebraic multiplicity = Geometric multiplicity for λ.
Dr. Anirban Lakshman (IIIT Kalyani)         MAC101                       26 / 35
                                      D IAGONALISATION
                                     
                       1  1 1
    Example: Let A = −1 −1 −1 .
                       0  0 1
  The characteristic equation of A is x 2 (1 − x) = 0.
  So, the eigen values of A are 0, 0, 1
       0 is an eigen value of algebraic multiplicity 2 and 1 is a simple
       eigen value of A (i.e., of algebraic multiplicity 1 ).
                                                                      
                                                                        1
       The eigen vectors corresponding to the eigen value 0 are c −1 ,
                                                                        0
       where c is a non-zero real number.
       ∴ So, The rank of eigen space corresponding to the eigen value 0
       is 1.
       Hence the geometric multiplicity of the eigen value 0 is 1.
       So, in this case G.M.≤ A.M.
Dr. Anirban Lakshman (IIIT Kalyani)         MAC101                    27 / 35
                                      D IAGONALISATION
                                                                     
                                                                    1
       The eigen vectors corresponding to the eigen value 1 are c −1 ,
                                                                    1
       where c is a non-zero real number.
       Hence the geometric multiplicity of the eigen value 1 is 1.
       So, in this case G.M. = A.M.
Dr. Anirban Lakshman (IIIT Kalyani)         MAC101                   28 / 35
                                      D IAGONALISATION
                                          Definition
     An n × n matrix A is said to be diagonalisable if A is similar to an
  n × n diagonal matrix.
       If A is similar to a diagonal matrix D = diag(λ1 , λ2 , . . . , λn ), then
       λ1 , λ2 , . . . , λn are the eigen values of A.
       If A is similar to a diagonal matrix D, then D = P −1 AP, where P is
       an non singular matrix.
Dr. Anirban Lakshman (IIIT Kalyani)          MAC101                                 29 / 35
                                      D IAGONALISATION
T HEOREM
     An n × n matrix A over a field F is diagonalisable iff ∃ n eigen
  vectors of A which are linearly independent.
T HEOREM
     Let A be an n × n matrix over a field F . If the eigen values of A be
all distinct and belong to F , then A is diagonalisable.
       The condition stated in this theorem is not necessary for matrix A
       to be diagonalisable
                                                
                                       3 2 1
       If we consider the matrix A = 2 3 1, then we show that
                                       0 0 1
       matrix A is diagonalisable but all the eigen values are not distinct.
Dr. Anirban Lakshman (IIIT Kalyani)         MAC101                       30 / 35
                                      D IAGONALISATION
                                          Defiition
     An eigen value λ is said to be regular if the G.M. of λ is equal to its
     A.M.
T HEOREM
     An n × n A is diagonalisable ⇐⇒ all its eigen values are regular.
Dr. Anirban Lakshman (IIIT Kalyani)          MAC101                      31 / 35
                                      D IAGONALISATION
    Example:Find                        −1
               a matrix Psuch that P AP is a diagonal matrix
                1 1 −2
    where A = −1 2 1 
                0 1 −1
    =⇒ The eigen values of A are 1, 2, −1
   The eigen vector
                  corresponding
                                  to the eigen values 1,2,-1 are
                 3        1        1
respectively c1 2 , c2 3 , c3 0 ; where c1 , c2 , c3 are arbitrary
                 1        1        1
non-zero real numbers.
    Since the eigen values are distinct, there are three linearly
independent eigen vectors of A, one corresponding to each eigen
value.                             
                        3    1          1
    The eigen vectors 2 , 3 and 0 are linearly independent.
                        1    1          1
Dr. Anirban Lakshman (IIIT Kalyani)         MAC101                         32 / 35
                                      D IAGONALISATION
                
            3 1 1
   Let P = 2 3 0 . Then P is a non singular matrix.
            1 1 1
Now,                                           
        1 1 −2 3 1 1            3 1 1       1 0 0
AP = −1 2 1  2 3 0 = 2 3 0 0 2 0  = PD
        0 1 −1 1 1 1            1 1 1       0 0 −1
     ⇒ P −1 AP = D = diag(1, 2, −1)
     So, A is a diagonal matrix.
Dr. Anirban Lakshman (IIIT Kalyani)         MAC101        33 / 35
                                      O UTLINE
1    E IGEN - VALUES ,E IGEN - VECTOR AND E IGEN SPACE
2    M INIMAL P OLYNOMIAL
3    R EFERENCES
Dr. Anirban Lakshman (IIIT Kalyani)     MAC101           34 / 35
                                      R EFERENCES
      Gilbert Strang, Linear Algebra and Its Applications.
      Steven J. Leon, Linear Algebra with Applications, Pearson.
      Carl D. Meyer, Matrix Analysis and Linear Algebra,Siam
      Kenneth Hoffman; Ray Kunze, Linear Algebra, Pearson
Dr. Anirban Lakshman (IIIT Kalyani)       MAC101                   35 / 35