6.17. Summary Theorem 6.1. m T tij diag 1 , , n T vk k vk (6.1) 6.2.1. Definition: Eigenvalue and Eigenvector. Eigen-equation T x x (6.2) is called an eigenvalue of T and x is an eigenvector belonging to . Theorem 6.2. The eigenvectors u1 , , uk belonging to a set of distinct eigenvalues 1 , , k of T are independent. Theorem 6.3. T : V V has at most n dimV distinct eigenvalues. eigenvalues 1 , , n , then m T diag 1, If T has exactly n distinct , n if we use the corresponding eigenvectors as basis. Theorem 6.4. Let V be a finite- dimensional linear space with complex scalars. Then every linear transformation T : V V has an eigenvalue. Theorem 6.5. Triangularization Theorem. Given any linear transformation T : V V , where V has complex scalars and dimV n . There is a basis for V relative to which m T is upper triangular. Furthermore, each diagonal element of m T is an eigenvalue of T. 6.7.1. Secular Equation det I A 0 (6.10) 6.7.2. Theorem 6.6. Let A aij be an n n matrix, then f det I A (6.10a) is a polynomial of degree n in . Furthermore, the coefficient of n is 1 and the constant term is f 0 det A det A . n 6.7.3. Characteristic Polynomials Definition: Characteristic Polynomial The determinant f det I A is called the characteristic polynomial of A. Theorem 6.7. The set of eigenvalues of T : V V consists of all the roots of the characteristic polynomial of m T that lie in the scalar field F of V. 6.9. Product And Sum n det A i i 1 n trA aii i 1 6.11.1. Theorem 6.8. If two n n matrices A and B represent the same linear transformation T, then there is a nonsingular matrix C such that B C 1 AC Furthermore, if A and B are the representations relative to the bases V v1, and U u1, , vn , un , respectively, then U VC . 6.11.2. Theorem 6.9. Let A and B be two n n matrices related by B C 1 AC , where C is n n and nonsingular. Then A and B represent the same linear transformation. 6.11.3. Definition Two n n matrices A and B are similar if there exists a nonsingular matrix C such that B C 1 AC . Theorem 6.10. Two n n matrices are similar iff they represent the same linear transformation. Theorem 6.11. Similar matrices have the same characteristic polynomial and hence the same eigenvalues. Theorem 6.12. Let W be an n-D linear space over the scalar field F and T : W W is a linear transformation. If the characteristic polynomial of T has n distinct roots 1 , , n in F, then (a) The corresponding eigenvectors u1 , (b) m T diag 1, , un form a basis for W. , n relative to the ordered basis U u1, (c) If m T A relative to another ordered basis V v1, , un . , vn , then C 1 AC , where C is the transition matrix given by U VC . 6.13.1. Theorem 6.13: Operators Cayley-Hamilton Theorem For Linear Given a characteristic polynomial for T : V V , n f i (6.24) i 1 Then n f T T i I O i 1 where O is the zero operator, i.e., f T x O Corollary 6.14: x V (6.25) Cayley-Hamilton Theorem For Matrices Let A be an n n matrix with characteristic polynomial n f det I A ck k k 0 Then n f A ck Ak O k 0 where O is the zero operator. 6.15.1. Definition: Jordan Block A Jordan block is a upper triangular n n matrix J jik such that jik 0 except jkk and for k 1, jk ,k 1 1 ,n where is a scalar. Some examples are 1 0 0 1 0 0 1 0 1 0 0 0 1 0 0 0 1 0 0 0 Theorem 6.15. A Jordan block J jik of order n has exactly one eigenvalue jkk and one independent eigenvector 1,0, ,0 . 6.15.2. Theorem 6.16: Jordan Normal Form Let V be an n-D linear space with complex scalars. Let T : V V be a linear transformation. Then there exists a basis for V relative to which m T diag J1, , Jm where each J k is a Jordan block. [ Block diagonal ]