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EIGENVALUES       AND   EIGENVECTORS
                                                                        DIAGONALIZATION SOME           SPECIAL TYPES
                                        CHAPTER 9                       OF   MATRICES


                                        Eigenvalues,


                                        Diagonalization,

                                        and Special

                                        Matrices

















                            9.1         Eigenvalues and Eigenvectors

                                        In this chapter, the term number refers to a real or complex number. Let A be an n × n matrix of
                                        numbers. A number λ is an eigenvalue of A if there is a nonzero n × 1matrix E such that
                                                                          AE = λE.                               (9.1)



                                          We call E an eigenvector associated with the eigenvalue λ.




                                           We may think of an n × 1 matrix of numbers as an n-vector, with real and/or complex
                                        components. If we consider A as a linear transformation mapping an n-vector X to an n-vector
                                        AX, then equation (9.1) holds when A moves E to a parallel vector λE. This is the geometric
                                        significance of an eigenvector.
                                           If c is a nonzero number and AE = λE, then

                                                                  A(cE) = cAE = cλE = λ(cE).
                                        This means that nonzero constant multiples of eigenvectors are eigenvectors (with the same
                                        eigenvalue).


                                 EXAMPLE 9.1

                                        Let

                                                                              10
                                                                         A =       .
                                                                              00
                                                                                                                  267

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