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Linear Algebra




                    Notes          If f is a complex-valued function whose domain includes c , ..., c , then
                                                                                 1    k
                                                            f(A) = f(c )E  + ... + f(c )E ;
                                                                   1  1      k  k
                                   in particular, A = c E  + ... + c E .
                                                 1  1     k  k
                                   We recall that an operator on an inner product space V is non-negative if T is self-adjoint and
                                   (T | )   0 for every   in V.
                                   Theorem 4: Let T be a diagonalizable normal operator on a finite-dimensional inner product
                                   space V. Then T is self-adjoint, non-negative, or unitary according as each characteristic value of
                                   T is real, non-negative, or of absolute value 1.
                                   Proof: Suppose T has the spectral resolution T = c E  + ... + c E , then T* =  c E  + ... +  c E . To say
                                                                          1  1    k  k        1  1     k  k
                                   T is self-adjoint is to say T = T*, or
                                                             (c  –  c )E  + ... + (c  –  c )E  = 0.
                                                              1   1  1     k   k  k
                                   Using the fact that E E  = 0 for i   j, and the fact that no E, is the zero operator, we see that T is
                                                   i  j                          j
                                   self-adjoint if and only if  c  =  c , j = 1, ... ,  k. To distinguish the normal operators which are
                                                         j   j
                                   non-negative, let us look at
                                                                   k       k
                                                         (T | ) =    c E  |  E i
                                                                      j j
                                                                  j  1    i  1

                                                               =     c j (E j  |E i  )
                                                                  i  j
                                                                          2
                                                                   c  E
                                                               =    j  j
                                                                  j
                                   We have used the fact that (E |E ) = 0 for i   j. From this it is clear that the condition (T | )  0
                                                          j  i
                                   is satisfied if and only if c    0 for each j. To distinguish the unitary operators, observe that
                                                       j
                                                            TT* = c c E  + ... + c c E .
                                                                  1 1  1   k k  k
                                                               =  c E  + ... + c E .
                                                                   2
                                                                            2
                                                                  1  1     k  k
                                                              2
                                                     2
                                   If TT* = I, then I = |c | E  + ... +  c E , and operating with E
                                                   1  1      k  k                 j
                                                                   2
                                                             Ej = c E .
                                                                  j  j
                                                     2
                                   Since E    0, we have  c  = 1 or  c  = l. Conversely, if  c  = 1 for  each j it is clear that TT* = I.
                                                                              2
                                        j            j      j                j
                                   It is important to note that this is a theorem about normal operators. If  T is a general linear
                                   operator on V which has real characteristic values, it does not follow that T is self-adjoint. The
                                   theorem states that if T has real characteristic values, and if T is diagonalizable and normal, then
                                   T is self-adjoint. A theorem of this type serves to strengthen the analogy between the adjoint
                                   operation and the process of forming the conjugate of a complex number. A complex number z
                                   is real or of absolute value 1 according as z =  z , or  z z = 1. An operator T is self-adjoint or unitary
                                   according as T = T* or T*T = I.
                                   We are going to prove two theorems now, which are the analogues of these two statements:
                                   1.  Every non-negative number has a unique non-negative square root.
                                   2.  Every complex number is expressible in the form ru, where r is non-negative and  u  = 1.
                                       This is the polar decomposition z = re  for complex numbers.
                                                                      i







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