Page 311 - Advanced Linear Algebra
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Metric Vector Spaces: The Theory of Bilinear Forms  295



            Suppose first that dim²:³ ~    and that : ~ span ² ³ . Since

                                    º  Á  »~º Á  »£


            Theorem 11.32 implies that there is a symmetry   for which     ~           where
                                                            =
                            ~f  . Hence,   is an isometry of   for which  ; ~ : and Theorem 11.9
            implies that  ;  ž  ~  ²  :   ž  ³  . Thus,  O    : ž  is the desired isometry.
            Now suppose the theorem is true  for  dim²:³      and  let  dim²:³ ~   .  Let
             ¢: ¦ ; be an isometry. Since  : is nonsingular, we can choose a nonisotropic
                                                     <
            vector  :  and write : ~ span ² ³ p <  , where   is nonsingular. It follows
            that
                                       ž
                              =~ : p : ~ span  ² ³ p < p : ž
            and
                                                       span
                            =~ ; p ;  ž  ~ ²    ² ³³ p < p ;  ž
            Now we may apply the one-dimensional case to deduce that
                                         ž

                                    <p : š <p ;     ž
            If       ž     ¢ < p: ¦ < p;  ž   is an isometry, then
                                    ž
                                                ž
                                  < p ²: ³~ ²< p : ³~ < p ; ž


            But       < š <    and since  dim ² <³ ~ dim ²<³    , the induction hypothesis

                              ž
                       ž

            implies that :š ²: ³ š ;  ž  .…
            As we have seen, Witt's extension theorem is a corollary of Witt's cancellation
            theorem.
                           (
            Theorem 11.35  Witt's extension  theorem) Let  =   and  =  Z  be isometric
            nonsingular orthogonal geometries over a field  , with char ²  -  ³  £     . Suppose
                                                    -
            that   is a subspace of   and
                               =
               <
                                             ¢< ¦ < ‹ =  Z
            is an isometry. Then   can be extended to an isometry from   to  =  Z .…

                                                            =
            Maximal Hyperbolic Subspaces of an Orthogonal Geometry
            We have seen that any orthogonal geometry   can be written in the form
                                                =
                                     =~ < p rad ²= ³
            where   is nonsingular. Nonsingular spaces are  better  behaved  than  singular
                  <
            ones, but they can still possess isotropic vectors.
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