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Chapter 5. Eigenvalues and Eigenvectors
                       82
                                                Recall that in Chapter 3 we discussed the matrix of a linear map
                                              from one vector space to another vector space. This matrix depended
                                              on a choice of a basis for each of the two vector spaces. Now that we are
                                              studying operators, which map a vector space to itself, we need only
                                              one basis. In addition, now our matrices will be square arrays, rather
                                              than the more general rectangular arrays that we considered earlier.
                                              Specifically, let T ∈L(V). Suppose (v 1 ,...,v n ) is a basis of V. For
                                              each k = 1,...,n, we can write
                                                                Tv k = a 1,k v 1 + ··· + a n,k v n ,
                        The k th  column of the  where a j,k ∈ F for j = 1,...,n. The n-by-n matrix
                        matrix is formed from                                        
                                                                       a 1,1  ...  a 1,n
                       the coefficients used to
                                                                       .          .  
                         write Tv k as a linear  5.11                  . .        . .  
                                                                    
                                                                                      
                       combination of the v’s.                         a n,1  ...  a n,n
                                              is called the matrix of T with respect to the basis (v 1 ,...,v n ); we de-

                                              note it by M T, (v 1 ,...,v n ) or just by M(T) if the basis (v 1 ,...,v n )
                                              is clear from the context (for example, if only one basis is in sight).
                                                                     n
                                                If T is an operator on F and no basis is specified, you should assume
                                              that the basis in question is the standard one (where the j th  basis vector
                                              is 1 in the j th  slot and 0 in all the other slots). You can then think of
                                              the j th  column of M(T) as T applied to the j th  basis vector.
                                                A central goal of linear algebra is to show that given an operator
                                              T ∈L(V), there exists a basis of V with respect to which T has a
                                              reasonably simple matrix. To make this vague formulation (“reasonably
                                              simple” is not precise language) a bit more concrete, we might try to
                                              make M(T) have many 0’s.
                                                If V is a complex vector space, then we already know enough to
                                              show that there is a basis of V with respect to which the matrix of T
                                              has 0’s everywhere in the first column, except possibly the first entry.
                                              In other words, there is a basis of V with respect to which the matrix
                                              of T looks like
                                                                                   
                           We often use ∗ to                            λ
                                                                                   
                        denote matrix entries                          0    ∗      
                                                                                    ;
                                                                                    
                                                                       .
                         that we do not know                           .           
                                                                       .
                            about or that are                                       
                                                                        0
                             irrelevant to the
                                              here the ∗ denotes the entries in all the columns other than the first
                             questions being
                                  discussed.  column. To prove this, let λ be an eigenvalue of T (one exists by 5.10)
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