Page 379 - Advanced Linear Algebra
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Tensor Products   363



            As we will see, there are other, more constructive ways to define the tensor
            product. Since we have adopted the universal pair definition, the other ways to
            define  tensor  product  are,  for us, constructions rather than definitions. Let us
            examine some of these constructions.

            Construction I: Intuitive but Not Coordinate Free
            The universal property for bilinearity captures the essence of bilinearity and the
            tensor map is the most “general” bilinear function on <d =  . To see how this
            universality can be achieved in a constructive manner, let ¸  “    0¹  be a basis

                                                                 !
               <
            for   and let     ¸  “       1  ¹     be a basis for  . Then a bilinear map   on  <  d  =   is
                                             =
            uniquely determined by assigning arbitrary values to the “basis” pairs ²  Á   ³


            and extending by bilinearity, that is, if "~        and # ~                   , then
                                                5
                        !²"Á #³ ~ !4     Á                 ~           !²  Á   ³



            Now, the tensor map  , being the most general bilinear map, must do this and
                              !
            nothing more. To achieve this goal, we define the tensor map   on the pairs
                                                                 !
            ²  Á  ³ in such a way that the images  !²  Á  ³ do not interact , and then extend




            by bilinearity.
            In particular, for each ordered pair  ²  Á   ³ , we invent a new formal symbol,


                        , and define   to be the vector space with basis
            written  n            ;
                                 : ~¸  n   “  0Á  1¹


                                                             and extending by

            The  tensor  map  is defined by setting  !²  Á   ³ ~   n


            bilinearity. Thus,
                                                5

                       !²"Á #³ ~ !4     Á                 ~           ²  n   ³


                                                         =
                                                    <
            To see that the pair ²;Á!³  is the tensor product of   and  , if  ¢< d = ¦ >   is
            bilinear, the universality condition  ~    k !  is equivalent to
                                    ²  n   ³ ~  ²  Á   ³




            which does indeed uniquely define a linear  map  ¢; ¦ >  . Hence, ²;Á!³  has
            the universal property for bilinearity and so we can write ;~ < n =   and refer
            to   as the tensor map.
              !
                                                     ;
            Note that while the set : ~¸  n   ¹  is a basis for   (by definition), the set


                                  ¸" n # “"<Á # = ¹
            of  decomposable  tensors spans  , but is not linearly independent. This does
                                       ;
            cause  some  initial  confusion  during the learning process. For example, one
            cannot define a linear map on  <n =   by assigning values arbitrarily  to  the
                                                                            is
            decomposable tensors, nor is it always easy to tell when a tensor    "n #
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