Page 144 - Curvature and Homology
P. 144

126     III.  RIEMANNIAN  MANIFOLDS:  CURVATURE,  HOMOLOGY

        B.  1-parameter local groups of  local transformations
        1.  Let P be  a point  on  the differentiable manifold  M  and  U  a  coordinate
        neighborhood of  P on which a vector field X # 0 is given.  Denote the com-
        ponents of X at P with respect to the natural basis in U by ti. There exists at P
        a  local coordinate system vl,---, vn such that  the  corresponding parametrized
        curves with v1 as parameter have at each point Q the vector XQ  as tangent vector.
        If  we put v1  = t, the equations
                         ui  = ui(v2, .-. , vn, t),  i = 1, *.. , n

        defining the coordinate transformations at P are the equations of  the 'integral
        curves'  (cf. I. D.8)  when the vi, i = 2, ..., n are regarded as constants and t as
        the parameter, that is, the coordinate functions ui, i = 1, ***,  n are solutions of
        the system of  differential equations




        with  ('(0)  = p, the  point  P corresponding to  t = 0.  More  precisely,  it  is
        possible to find a neighborhood U(Q) of Q and a positive number E(Q) for every
       Q E U such that  the system (*) has a solution for  I t 1  < a(Q).  Denoting this
        solution by
                      ut(v2,  , vn, t) = exp (tX)ui(v2, ... , vn, 0)
       show that


       provided both sides are defined. In this way,  we see that the 'exp'  map defines
       a local 1-parameter group exp(tX) of (local) transformations.
       2.  Conversely, every 1-parameter local group of local transformations tp,  may be
       so defined. Indeed, for every P E M put



       and consider the vector field X defined by the initial conditions




       (or, rYp = (dP(t)/dt),,,).  It follows that



       3.  The map exp(tX) is defined on  a neighborhood U(Q) for  I  t I < c(Q) and
       induces a map exp(tX),  which is an isomorphism of  Tp onto Tp(,,-the  tangent
   139   140   141   142   143   144   145   146   147   148   149