Page 395 - Advanced Linear Algebra
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Tensor Products   379



            Change of Base Field
            The tensor product provides a convenient way to extend the base  field  of  a
            vector space that is more general than the complexification of a real vector
            space, discussed earlier in the book. We refer to a vector space over a field   as
                                                                         -
            an  -space  and write  - .
              -
                              =
            Actually, there are several approaches to “upgrading” the base field of a vector
            space. For instance, suppose that   is an extension field of  , that is,  -  ‹  2  .
                                       2
                                                             -
            If ¸  ¹  is a basis for = -  , then every %  = -   has the form

                                       %~

            where   - . We can define a 2  -space = 2   simply by taking all formal linear

            combinations of the form

                                       %~
                                                      2
            where      . Note that the dimension of  2 2  =   as a  -space is the same as the
                                                          (
                                                   -
            dimension of  -  =   as an  -space. Also,  2  -  =   is an  -space  just restrict the scalars
            to  -   and as such, the inclusion  map   )  ¢  =  -  ¦  =  2    sending  %    =  -    to
             ²%³ ~ %  = 2  is an  -monomorphism.
                             -
            The approach described in the previous paragraph  uses  an  arbitrarily  chosen
                       and is therefore not coordinate free. However, we  can  give  a
            basis for  = -
            coordinate-free approach using tensor products as follows. Since 2  is a vector
            space over  , we can form the tensor product
                     -
                                     >~ 2 n = -  -
                                       -
                                             -
            It is customary to include the subscript   on  n  -  to denote the fact that the
            tensor product is taken with respect to the base field  . (All relevant maps are
                                                        -
                                              =
            -           --bilinear and  -linear.) However, since  -   is not a  2  -space, the only tensor
                                                  -
            product of 2   and =  -  that makes sense is the  -tensor product and so we will
            drop the subscript  .
                           -
            The tensor product >   is an  -space by definition of tensor product, but we
                                     - -
                           2
            can make it into a  -space as follows. For       2  , the temptation is to “absorb”
            the scalar   into the first coordinate,

                                     ²n #³ ~ ²   ³ n #
            but we must be certain that this is well-defined, that is,
                           n# ~    n$   ¬    ²   ³ n# ~ ²   ³n$
            But for a fixed  , the map       ²Á #³ ª ²     ³ n #  is bilinear and so the universal

            property of tensor products implies that there is  a  unique  linear  map
                      n# ª ²     ³n#, which we define to be scalar multiplication by  .
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