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Richa Nandra, Lovely Professional University  Unit 12: Introduction and Characteristic Values of Elementary Canonical Forms





                Unit 12: Introduction and Characteristic Values of                              Notes
                             Elementary Canonical Forms



            CONTENTS
            Objectives
            Introduction

            12.1 Overview
            12.2 Characteristic Values
            12.3 Summary
            12.4 Keywords

            12.5 Review Questions
            12.6 Further Readings

          Objectives

          After studying this unit, you will be able to:

              Know that when the matrix of the linear transformation is in the diagonal form for some
               ordered basis the properties of the transformation can be seen at a glance.
              See that a matrix A of a linear operator T can be cast into a diagonal form under similarity
               transformations.
                                   –1
              See that a matrix A and P  AP where P is an invertible have the same characteristic values.
          Introduction

          In this unit it is shown how a matrix has a diagonal form.

          For this purpose the characteristic values and characteristic vectors  are worked out and an
          invertible matrix is  worked out of the characteristic vectors  that can  diagonalize the  given
          matrix.

          12.1 Overview


          One of our primary aim in these units is to study linear transformation on finite dimensional
          vector spaces. So far we have studied many specific properties of linear transformations.  In
          terms of ordered basis vectors we have represented such types of matrices by matrices. In terms
          of matrices we  see lots of insight of the linear transformation. We also  explored the linear
          algebra L(V, V) consisting of the linear transformations of a space into itself.
          In the next few units we shall concentrate ourselves with linear operators on a finite dimensional
          vector space. If we consider the ordered basis   = ( ,  ,...  ) then the effect of T on   is
                                                    1  2   n                    i
                                           n
                                     T      A
                                        i     ji  j  i = 1, 2, ... n
                                          j  1
          where the new ordered basis is   = ( ,  , ...  ) . If we now choose the basis   = (  ,  , ...  ) in
                                        1  2   n                            1  2   n
          such a way that



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