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Metric Vector Spaces: The Theory of Bilinear Forms  279




            invariants under congruence and that the set of all matrices of the form ?   Á c
            is a set of canonical forms.
            Witt's Extension and Cancellation Theorems
            We now prove the Witt theorems for symplectic geometries.

                           (
            Theorem 11.15  Witt's extension  theorem) Let  =   and  =  Z  be isometric
            nonsingular symplectic geometries over a field  . Then any isometry
                                                  -
                                             ¢: ¦ : ‹ =  Z
            on a subspace   of   can be extended to an isometry from   to  =  Z .
                        :
                            =
                                                           =
            Proof. According to Theorem 11.12, we can extend   to  a  nonsingular

            completion of  , so we may simply assume that   and  :  :       are  nonsingular.
                        :
            Hence,
                                       =~ : p : ž
            and
                                      Z


                                     =~ : p ² :³  ž
            To complete the extension of   to  , we need only choose a hyperbolic basis
                                       =

                                     ²  Á  ÁÃÁ  Á  ³




            for : ž  and a hyperbolic basis
                                                  Z
                                       Z
                                         Z
                                               Z
                                     ²  Á  ÁÃÁ  Á  ³




            for ²:³ ž   and define the extension by setting    ~   Z      and    ~      Z  .…





            As a corollary to Witt's extension theorem, we have Witt's cancellation theorem.
                          (
            Theorem 11.16  Witt's cancellation theorem) Let  =   and  =  Z   be  isometric
            nonsingular symplectic geometries over a field  . If
                                                  -
                                                 Z
                              =~ : p : ž  and  = ~ ; p ;  ž
            then
                                              ž
                                    :š ; ¬ : š ;   ž                      …
            The Structure of the Symplectic Group: Symplectic Transvections
            Let us examine the nature of symplectic  transformations (isometries) on a
            nonsingular symplectic geometry  =  . Recall that for  a  real  vector  space,  an
            isometric isomorphism, which corresponds to an isometry in the present context,
            is the same as an orthogonal map and  orthogonal  maps  are  products  of
                                                                is defined as an
            reflections (Theorem 10.17). Recall also that a reflection / #
            operator for which
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