Page 102 - Linear Algebra Done Right
P. 102

dim V vectors in V is a basis of V (see 2.17); thus (v 1 ,...,v dim V ) is a
                      basis of V. With respect to this basis consisting of eigenvectors, T has
                      a diagonal matrix.       Diagonal Matrices                                            89
                         We close this section with a proposition giving several conditions
                      on an operator that are equivalent to its having a diagonal matrix with
                      respect to some basis.


                      5.21   Proposition:  Suppose T ∈L(V). Let λ 1 ,...,λ m denote the   For complex vector
                      distinct eigenvalues of T. Then the following are equivalent:       spaces, we will extend
                                                                                          this list of equivalences
                      (a)   T has a diagonal matrix with respect to some basis of V;      later (see Exercises 16
                      (b)   V has a basis consisting of eigenvectors of T;                and 23 in Chapter 8).
                      (c)   there exist one-dimensional subspaces U 1 ,...,U n of V, each in-
                            variant under T, such that

                                                 V = U 1 ⊕· · ·  U n ;

                      (d)   V = null(T − λ 1 I) ⊕· · ·  null(T − λ m I);
                      (e)   dim V = dim null(T − λ 1 I) + ··· + dim null(T − λ m I).


                         Proof: We have already shown that (a) and (b) are equivalent.
                         Suppose that (b) holds; thus V has a basis (v 1 ,...,v n ) consisting of

                      eigenvectors of T. For each j, let U j = span(v j ). Obviously each U j
                      is a one-dimensional subspace of V that is invariant under T (because
                      each v j is an eigenvector of T). Because (v 1 ,...,v n ) is a basis of V,
                      each vector in V can be written uniquely as a linear combination of
                      (v 1 ,...,v n ). In other words, each vector in V can be written uniquely
                      as a sum u 1 +· · ·+ u n , where each u j ∈ U j . Thus V = U 1 ⊕ ··· ⊕ U n .
                      Hence (b) implies (c).
                         Suppose now that (c) holds; thus there are one-dimensional sub-
                      spaces U 1 ,...,U n of V, each invariant under T, such that

                                              V = U 1 ⊕ ··· ⊕ U n .

                      For each j, let v j be a nonzero vector in U j . Then each v j is an eigen-
                      vector of T. Because each vector in V can be written uniquely as a sum
                      u 1 +· · ·+u n , where each u j ∈ U j (so each u j is a scalar multiple of v j ),
                      we see that (v 1 ,...,v n ) is a basis of V. Thus (c) implies (b).
   97   98   99   100   101   102   103   104   105   106   107