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242                                                                               Diagonalization


                               Suppose that V is any n-dimensional vector space. We call a linear trans-
                            formation L: V 7→ V diagonalizable if there exists a collection of n linearly
                            independent eigenvectors for L. In other words, L is diagonalizable if there
                            exists a basis for V of eigenvectors for L.
                               In a basis of eigenvectors, the matrix of a linear transformation is diag-
                            onal. On the other hand, if an n × n matrix is diagonal, then the standard
                            basis vectors e i must already be a set of n linearly independent eigenvectors.
                            We have shown:

                            Theorem 13.1.1. Given an ordered basis B for a vector space V and a
                            linear transformation L: V → V , then the matrix for L in the basis B is
                            diagonal if and only if B consists of eigenvectors for L.


                                                Non-diagonalizable example




                                                        Reading homework: problem 1


                               Typically, however, we do not begin a problem with a basis of eigenvec-
                            tors, but rather have to compute these. Hence we need to know how to
                            change from one basis to another:



                            13.2      Change of Basis

                                                                                                0
                                                                                          0
                                                                                                        0
                            Suppose we have two ordered bases S = (v 1 , . . . , v n ) and S = (v , . . . , v )
                                                                                                1      n
                                                                 0
                            for a vector space V . (Here v i and v are vectors, not components of vectors
                                                                 i
                                                                   0
                            in a basis!) Then we may write each v uniquely as
                                                                   k
                                                                 X
                                                             0
                                                                        i
                                                            v =      v i p ,
                                                                        k
                                                             k
                                                                  i
                                    0
                            this is v as a linear combination of the v i . In matrix notation
                                    k
                                                                           p    p   · · · p
                                                                            1   1        1  
                                                                             1   2        n
                                                                         p  2 1  p 2 2    
                                            0
                                         0
                                        v , v , · · · , v 0                              .
                                                                                           
                                         1  2       n  = v 1 , v 2 , · · · , v n   .    .
                                                                          . .           . . 
                                                                           p n      · · · p n
                                                                            1             n
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