Page 308 - Advanced Linear Algebra
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292    Advanced Linear Algebra




                                       !


                                             8
                                     ´µ 4´µ ~ 4 8
                                          8
                                       8
            Taking determinants gives
                                det²4 ³ ~  det²´ µ ³   det²4 ³
                                                       8
                                     8
                                               8
            Therefore, if   is nonsingular, then
                      =
                                      det²´ µ ³ ~ f
                                           8
            Since the determinant is  an  invariant under similarity, we have the following
            theorem.
            Theorem 11.31  Let    be an orthogonal transformation on a nonsingular

            orthogonal geometry  .
                             =

                                                       =
            1  )det²´ µ ³  is the same for all ordered bases   for   and
                                                  8 8
                                       det²´ µ ³ ~ f
                                             8
               This determinant is called the determinant  of   and denoted by det²³ .


             )

            2   If  det²³ ~   , then   is called a  rotation  and if  det²³ ~ c  , then   is



               called a reflection .
            3   The set E  )  b   of rotations is a subgroup of the orthogonal group E ²= ³  ²= ³
               and  the determinant map  det¢²= ³ ¦ ¸c Á  ¹  is an epimorphism with
                                         E
               kernel  E  b  . Hence, if char ²-³ £   , then  E ²= ³  b  ²= ³  is a normal subgroup

               of E²= ³  of index  .…
            Symmetries
                                                                is defined as an
            Recall again that for a real inner product space, a reflection / "
            operator for which
                            /" ~ c"Á /$ ~ $ for all  $  º"» ž
                              "
                                        "
            and that
                                               º%Á "»
                                    /% ~ % c        "
                                     "
                                              º"Á "»
            In  particular, if  char²-³ £    and  "  =   is nonisotropic, then  span²"³  is
            nonsingular and so
                                  = ~ span ²"³ p span ²"³ ž
                               is well-defined and, in the context of general orthogonal
            Then the reflection / "
            geometries, is called the symmetry  determined by   and we will denote it by
                                                      "
                                "  " . We can also write   ~c p     , that is,

                                      " ²% b&³ ~ c% b&
            for all % span ²"³  and &  span ²"³ ž .
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