Page 410 - Advanced Linear Algebra
P. 410

394    Advanced Linear Algebra



            in the sum for  . For example, if
                        #



                        # ~   n  n  b   n  n  b  n  n




            then

                           . ¸ Á Á ¹ ²#³ ~ ¸ n  n   Á  n  n   ¹





                                                   #
            Let  :²#³   denote  the sum of the terms of   associated with  . ²#³ . For
                                                                    4
                 4
            example,

                          : ¸ Á Á ¹ ²#³ ~   n  n  b   n  n



            Thus,   can be written in the form
                 #
                                               p         s
                              #~    : ²#³ ~    4         ! !
                                  4          4  q  !. ²#³  t
                                                   4
            where the sum is over a collection of multisets  4   with  :  ²  #  ³  £ 4     . Note also
                               4 £
            that   !   since !. ²#³ . Finally, let
                                    "  ~ 4        n    Ä  n
                                                           .

            be the unique member of . 4   for which     Ä
            Now we can get to the business at hand.
            Symmetric and Antisymmetric Tensors

            Let :    be the symmetric group on ¸ Á à Á  ¹ . For each   :   , the multilinear

            map  ¢ =  d   ¦ ; ²= ³  defined by

                                 ²% Á Ã Á % ³ ~ %               nÄn%

            determines a unique linear operator      on ;²= ³  for which
                                                  ²% nÄn% ³ ~ %    n Än%
            For example, if  ~    and  ~ ²   ³ , then

                                ²  ³ ²# n# n# ³ ~ # n# n#





            Let ¸  ÁÃÁ  ¹  be a basis for  . Since      is a bijection of the basis
                                    =


                                8                            8 ~¸  n Ä n   “    ¹

            it follows that      is an isomorphism of  ;²= ³ . Note also that            is  a
            permutation of each  .  , that is, the sets  . 4  4   are invariant under     .
            Definition Let   be a finite-dimensional vector space.
                        =
   405   406   407   408   409   410   411   412   413   414   415