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Linear Algebra




                    Notes          An example of a self-adjoint algebra is L(V, V) itself. Since the intersection of any collection of
                                   self-adjoint algebras is again a self-adjoint algebra, the following terminology is meaningful.
                                   Definition: If  is a family of linear operators on a finite-dimensional inner product space, the
                                   self-adjoint algebra generated by  is the smallest self-adjoint algebra which contains  .
                                   Theorem 8:  Let    be a  commuting  family  of  diagonalizable normal  operators  on  a  finite-
                                   dimensional inner product space V, and let  be the self-adjoint algebra generated by  and the
                                   identity operator. Let {P ,..., P } be the resolution of the identity defined by . Then  is the set
                                                      1   k
                                   of all operators on V of the form
                                                                  k
                                                                    c P
                                                                     j j
                                                              T =                                         … (15)
                                                                 j  1
                                   where c , ..., c  are arbitrary scalars.
                                         1   k
                                   Proof: Let  denote the set of all operators on V of the form (15). Then  contains the identity
                                   operator and the adjoint

                                                             T* =   c P
                                                                    j j
                                                                  j
                                   of each of its members. If T =   c P   d P  , then for every scalar a
                                                              j j  and U =
                                                                           j j
                                                            j            j
                                                         aT + U =   (ac  d j  )P j
                                                                  j
                                   and

                                                            TU =    c d P P
                                                                     i j i j
                                                                  , i j
                                                               =   c d P
                                                                    i j j
                                                                  j
                                                               = UT.

                                   Thus  is a self-adjoint commutative algebra containing  and the identity operator. Therefore
                                    contains .
                                   Now let r , ..., r  be all the roots of . Then for each pair of indices (i, n) with i   n, there is an
                                          1    k
                                   operator T  in  such that r (T )   r (T ). Let a  = r (T ) – r (T ) and b  = r (T ). Then the linear
                                           in            i  in  n  in   in  i  in  n  in  in  n  in
                                   operator
                                                             Q =   II a  1   (T  – b I)
                                                              i      in   in  in
                                                                  n i
                                   is an element of the algebra . We will show that Q  = P  (1   i   k). For this, suppose j   i and that
                                                                           i   i
                                     is an arbitrary vector in V(r ). Then
                                                          j
                                                            T  = r (T )
                                                             ij   j  ij
                                                               = b
                                                                  ij
                                   so that (T  – b I)  = 0. Since the factors in Q  all commute, it follows that Q  = 0. Hence Q  agrees
                                          ij  ij                     i                       1           i
                                   with P  on V(r ) whenever j   i. Now suppose   is a vector in V(r ). Then T   = r (T )  and
                                        i     j                                       i       in  i  in  j
                                                        a  –1 (T  – b I)  = a  –1 [r (T ) – r (T )]  =  .
                                                         in  in  in    in  i  in  n  in
                                   Thus Q  =   and Q  agrees with P  on V(r ); therefore, Q  = P  for -i = 1, ... , k. From this it follows
                                        i         i           i     i          i  i
                                   that  = .


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