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Linear Algebra




                    Notes          29.1 Spectral Theory

                                   In this unit we try to implement the findings of the Theorems 9 and 13 of unit 26 regarding the
                                   diagonalization of self-adjoint and normal operators.

                                   We start with the following spectral theorem:
                                   Theorem 1 (Spectral Theorem): Let T be a normal operator on a finite dimensional complex inner
                                   product space V or a self-adjoint operator on a finite dimensional real inner product space. Let
                                   C , ... C  be the distinct characteristic values of T. Let W  be the characteristic space associated with
                                    1   k                                    j
                                   C  and E , the orthogonal projection of V on W . Then W  is orthogonal to W*  when i   j, V is the
                                    j    j                             j       i               j
                                   direct sum of W , W , ... W  and
                                               1  2    k
                                                              T = C E  + C E  + ... + C  E                 ...(1)
                                                                  1  1  2  2    k  k
                                   Proof:  Let   be a vector in W ,   a vector in W , and suppose i   j. Then  c,( | ) = (T | ) =
                                                            j             i
                                   ( |T* ) =  ( |c i  ).  Hence (c  – c )( | ) = 0, and since. c  – c    0, it follows that ( | ) = 0. Thus W j
                                                                              j
                                                                                 i
                                                            i
                                                         j
                                   is orthogonal to  W , when  i   j. From the fact that  V has an orthonormal basis consisting of
                                                  i
                                   characteristic vectors (cf. Theorems 9 and 13 of  unit 26), it follows that V = W  + ... + W . If
                                                                                                  1       k    j
                                   belongs to V  (1   j   k) and   + ... +   = 0, then
                                             j            1      k
                                                              0 =  ( |  j )  ( |  j )
                                                                   i
                                                                               i
                                                                     j      j
                                                                    2
                                                               =   i
                                   for every i, so that V is the direct sum of W , ... , W . Therefore E  + ... + E  = I and
                                                                     1     k         1      k
                                                              T = TE  + ... + TE .
                                                                   1       k
                                                               = c E  + ... + c E
                                                                  1  1    k  k
                                   The decomposition (1) is called the spectral resolution of T. This terminology arose in part from
                                   physical applications which caused the spectrum of a linear operator on a finite-dimensional
                                   vector space to be defined as the set of characteristic values for the operator. It is important to
                                   note that the orthogonal projections E , ... , E  are canonically associated with T; in fact, they are
                                                                 1    k
                                   polynomials in T.
                                                     x  c i
                                   Corollary: If e  =   II  , then E  = e (T) for 1   j   k.
                                              j                  j  j
                                                 i  j c j  c i
                                   Proof: Since E E  = 0 when i   j, it follows that
                                              i  j
                                                                  2
                                                                          2
                                                             T = c E  + ... + c E
                                                              2
                                                                  1  1    k  k
                                   and by all easy induction argument that
                                                             T = c E  + ... + c E
                                                                          n
                                                                  n
                                                              n
                                                                  1  1    k  k
                                   for every integer n   0. For an arbitrary polynomial
                                                                  r    n
                                                              f =    n x
                                                                 n  0
                                   we have
                                                                  r    n
                                                            f(T) =   n T
                                                                 n  0





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