Page 45 - Introduction to Statistical Pattern Recognition
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2  Random Vectors and their Properties                        27



                     is called an eigenvector-. When X is a symmetric n x n matrix, we haven real eigen-
                     values  XI,. . ., h,  and  n  real  eigenvectors  $,,  . . . , @,.  The  eigenvectors
                     corresponding to two different eigenvalues are orthogonal.  This can be proved as
                     follows: For h,, @, and h,, @,(A, #A,),

                                        X@, =A,@,  and  XQJ = A,@,  .           (2.76)
                     Multiplying the first equation by @;,   the second by $7, and subtracting the second
                     from the first gives

                                      ('1   - 'J)@T@, = @;'$I   -   =   9       (2.77)
                     since  C is a symmetric matrix.  Since h, +AJ,

                                                                                (2.78)
                                                 OT@I  = 0 '
                     Thus, (2.73), (2.74), and (2.78) can be rewritten as

                                                                                (2.79)

                                                                                (2.80)

                     where Q, is an n x n matrix, consisting of n eigenvectors as

                                              @ = [@I   '  '  '  4411           (2.81)
                     and A is a diagonal matrix of eigenvalues as
                                                 F'      0



                                                                                (2.82)





                     and I is the identity matrix.  The matrices 0 and A will be called the eigenvector
                     matrix and the eigenvalue matrix, respectively.
                          Let us use @ as the transformation matrix A of (2.61) as
                                                Y=OTX.                          (2.83)

                     Then, from (2.63),
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