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9.3:  Bilinear Forms                  335

            The point that  has emerged  from the preceding  discussion
        is that  matrices  which  represent  the  same  bilinear  form  with
        respect  to  different  bases  of  the  vector  space  are  congruent.
        This  result  is to  be  compared  with  the  fact  that  the  matrices
        representing  the  same  linear  transformation  are  similar.
            The  conclusions  of  the  the  last  few  paragraphs  are  sum-
        marized  in the  following  basic  theorem.

        Theorem     9.3.1
        (i)  Let  f  be a  bilinear form  on  an n-dimensional  vector  space
        V  over  a field  F  and  let  B  =  {vi,...,  v n }  be an  ordered basis
        of  V.  Define  A  to  be  the  n  x  n  matrix  whose  (i,j)  entry  is
        /(v»,  Vj);  then

                                            T
                           /(u,v)  =  ([u] B ) A[v] B ,

        and  A  is  the  n  x  n  matrix  representing  f  with  respect  to  B.
        (ii)  If  B'  is  another  ordered  basis  of  V,  then  f  is  represented
        with  respect to B'  by the  matrix  S T  AS  where S  is  the  invertible
        matrix  describing  the  basis  change  B'  —>  B.
        (iii)  Conversely,  if  A  is  any  n  x  n  matrix  over  F,  a  bilinear
        form  on  V  is  defined  by  the  rule (u, v)  =  ([U]B) A[V]B-  It
                                                            T
                                           /
        is  represented  by  the  matrix  A  with  respect  to  the  basis  B.
        Symmetric     and  skew-symmetric      bilinear  forms
             A bilinear  form  /  on  a vector  space  V  is called  symmetric
        if  its  values  are  unchanged  by  reversing  the  arguments,  that
        is,  if
                               /(u,v)  =  /(v,u)

        for  all  vectors  u  and  v.  Similarly,  /  is  said  to  be  skew-
        symmetric  if
                              /(u,v)  =  - / ( v , u )

                                                    /
        is  always  valid.  Notice  the  consequence, (u,  u)  =  0  for  all
        vectors u.  For example,  any real inner  product  is a  symmetric
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