Page 411 - Advanced Linear Algebra
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Tensor Products   395



             )

            1   A tensor !; ²= ³  is symmetric  if
                                               !~!
                                      . The set of all symmetric tensors
               for all permutations   :

                          :; ²= ³ ~ ¸!  ; ²= ³ “       ! ~ ! for all        : ¹


               is a subspace of ;²= ³ , called the symmetric tensor space  of degree
               over .
                   =
             )

            2   A tensor !; ²= ³  is antisymmetric  if

                                            !~²c ³ !
               The set of all antisymmetric tensors


                       (; ²= ³ ~ ¸!  ; ²= ³ “       ! ~ ²c ³ ! for all        : ¹


               is a subspace of ;²= ³ , called the antisymmetric tensor space  or exterior
               product space of degree   over  .…
                                         =

            We can develop the theory of symmetric and antisymmetric tensors in tandem.
            Accordingly,  let us write (anti)symmetric to denote a tensor that is either
            symmetric or antisymmetrtic.
                                                            taking   to  , an

                                                                        !
            Since  for any   Á !  . 4  , there is a permutation
            (anti)symmetric tensor   must have  .  4  ²  #  ³  ~  .  4   and so
                              #
                               #~    : ²#³ ~    4  8        ! !  9
                                   4          4   !. 4

                                                   # 4
            Since      is a permutation of .  , it follows that   is symmetric if and only if
                                        ²: ²#³³ ~ : ²#³
                                                 4
                                        4
            for all      and this holds if and only  if  the  coefficients    :    !    of  : ²#³   are
                                                                     4
            equal, say       !  4 ~   for all    !  .  4  . Hence, the symmetric tensors are precisely
            the tensors of the form
                                    #~    8         ! 9 4
                                        4      !. 4
            The tensor   is antisymmetric if and only if
                     #

                                     ²: ²#³³ ~ ²c ³ : ²#³               (14.4)
                                                   4
                                     4
            In this case, the coefficients   of  4  :²#³  differ only by sign. Before examining
                                     !
            this more closely, we observe that  4   must be a set. For if  4   has an element
            of multiplicity greater than  , we can split  .  4   into two disjoint parts:
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