Page 121 - Curvature and Homology
P. 121

Equation (3.5.2) indicates a (local) relationship between the derivations
       B(X) and d. Indeed, if  we write
                         1
                      dd =-cikCUj  A &Jk,  cifk f cij =O       (3.5.3)
                            2
       and
                      @(Xj)  x, = - bif,  X*,  b:,  + b:,  = 0,   (3.5.4)
       where  {X*} and {uk) are dual bases, then



       from which by (1.5.1),  (3.5.3) and (3.5.4)



       The reader is referred to Chapter IV where this relationship is exploited
       more fully. We remark that equation (3.5.2) has important implications
       in the theory  of  connections as well  [63].



                    3.6.  Lie transformation groups  [TI, 631
         A  Lie poup  G  is  a group  which is  simultaneously  a  differentiable
       manifold (the points of the manifold coinciding with the elements of the
       group)  in  which  the  group  operation  (a, b) -+ ab-I  (a, b  E G)  is  a
       differentiable map of  G x  G into G. It is well-known that as a manifold
       G admits an analytic structure in such a way that the group operations
       in G are analytic. It follows that the map x -+ ax is analytic. We denote
       this map by La and call it the left  translation in  G by  a.  Hence, every
       left translation La is an  analytic homeomorphism of  G (as an analytic
       manifold) with  itself.  It follows that  if  x  and y  are  any  two  elements
       of  G,  there  exists  an  element  a = yx-I  such  that  the  induced  map
       La.  = (La), maps T, isomorphically onto  T,.
         An  infinitesimal transformation  X  on  G  is  said to  be  left  invariant
       if for every a€ G,  La  ,Xe = X,.  Hence, associated with an element AE Te,
       where  e E G  is  the  identity,  there  is  a  unique  left  invariant  infini-
       tesimal transformation X which takes the value A at e. It can be shown
       that  every left invariant infinitesimal transformation  is analytic.  Let fi
       denote  the  set  of  left  invariant  infinitesimal  transformations  of  G;
       L is a vector space over R  of  dimension equal to that of  G.  In fact, if
       to a tangent vector Xe E Te we associate the infinitesimal transformation
       X EL defined by  Xu = La,Xe  (a E G) it is seen  that as vector  spaces
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