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Linear Algebra




                    Notes
                                   based upon the observation that complex conjugation has the properties  (z  z  )  =  z  z  ,(z z  )
                                                                                             1   2   1   2  1 2
                                        ,
                                   =  z z z  = z. One must be careful to observe the reversal of order in a product, which the adjoint
                                     1 2
                                   operation imposes: (UT)* = T*U*. We shall mention extensions of this analogy as we continue
                                   our study of linear operators on an inner product space. We might mention something along
                                   these lines now. A complex number z is real if the only if  z  . z  One might expect that the linear
                                   operators T such that T = T* behave in some way like the real numbers. This is in fact the case. For
                                   example, if T is a linear operator on a finite-dimensional complex inner product space, then
                                                              T = U  + iU
                                                                    1    2
                                   where U  = U* and U = U*. Thus, in some sense, T has a ‘real part’ and an ‘imaginary part.’ The
                                         1   1     2   2
                                   operators U  and U  satisfying U  = U*, and U = U*, and are unique, and are given by
                                            1     2          1   1     2   2
                                                                    1
                                                             U   =   (T T *)
                                                               1    2
                                                                    1
                                                             U   =   (T T *).
                                                               2    2i
                                   A linear operator T such that T = T* is called self-adjoint (for Hermitian). If  is an orthonormal
                                   basis for V, then

                                                            [T*]  = [T]*
                                                                    
                                   and so T is self-adjoint if and  only if its matrix in every  orthonormal basis is a self-adjoint
                                   matrix. Self-adjoint operators are important, not simply because they provide us with some sort
                                   of real  and imaginary  part for  the general  linear operator,  but  for  the  following  reasons:
                                   (1) Self-adjoint operators have many special properties. For example, for such an operator there
                                   is an orthonormal basis of characteristic vectors. (2) Many operators which arise in practice are
                                   self-adjoint. We shall consider the special properties of self-adjoint operators later.

                                   Self Assessment


                                   1.  Let V be a finite-dimensional inner product space T a linear operator on V. If T is invertible,
                                       show that T* is invertible and (T*)  = (T )*.
                                                                   –1
                                                                        –1
                                   2.  Show that the product of two self-adjoint operators is self-adjoint if any only if the two
                                       operators commute.

                                   25.3 Summary

                                      The linear functional  f concept is also a form  of inner product on a finite-dimensional
                                       inner product space.
                                      The fact that f has the form f( ) = (  ) for some   in V helps us to prove the existence of the
                                       ‘adjoint’ of a linear operator T on V.

                                      A linear operator T  such that  T =  T* is called  self-adjoint (or  Hermitian)  and so  T  is
                                       self- adjoint if and only if its matrix in every orthonormal basis is a self-adjoint matrix.

                                   25.4 Keywords


                                   A linear functional f on a finite dimensional inner product space is ‘inner-product with a fixed
                                   vector in the space’. Let   be some fixed vector in any inner product space V, we then define a
                                   function f  from V into the scalar field by




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