Page 43 - Curvature and Homology
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1.7.  AFFINE  CONNECTIONS              25
        The covariant derivative  of  a tensor field being itself  a tensor field, we
        may  speak  of  second  covariant  derivatives,  etc.,  the result  again  being
        a tensor  field.
         Since  Euclidean  space  En,  considered  as  a  differentiable manifold,
        is  covered  by  one  coordinate  neighborhood,  it  is  not  essential  from
        our  point  of  view  to  introduce  the  concept  of  covariant  derivative.
       In  fact,  the  affine  connection  is  defined  by  setting  the  rJ;  equal  to
       zero.  The  underlying  affine  space  An  is  the  ordinary  n-dimensional
       vector  space-the   tangent  space  at  each  point  P  of  En  coinciding  '
       with  An.  Indeed, the  linear  map  sending the  tangent  vector  a/aud to,
       the vector  (0, ..., 0, 1,0, ..., 0) (1 in the zTh  place)  identifies  the tangent
       space  Tp with An itself.  Let P and Q be two  points  of  An. A tangent
       vector at P and one at Q are said to be parallel if they may be identified
       with  the  same  vector  of  An.  Clearly,  the  concept  of  parallelism  (of
       tangent  vectors)  in  An  is  independent  of  the  curve  joining  them.
       However,  in general,  this  is not  the case  as  one readily  sees from the
        differential geometry of  surfaces in E3. We therefore make the following
       definition:
         Let C = C(t) be a piecewise differentiable curve in M.  The tangent
       vectors




       are said to be parallel along C if  the covariant derivative  DX(t) of  X(t)
       vanishes in the direction of  C, that is, if





       A  piecewise  differentiable  curve  is  called  an  auto-parallel curve,  if  its
       tangent  vectors are parallel  along  the curve itself.
         The  equations  (1.7.14)  are  a  system  of  n  first  order  differential
       equations, and so corresponding to the initial value X  = X(to) at t = to
       there is a unique  solution.  Geometrically,  we say that the vector X(t,)
       has been given a parallel displacement along C. Algebraically, the parallel
       displacement along C is a linear  isomorphism  of  the  tangent  spaces  at
       the  points of  C. By definition, the auto-parallel curves are the integral
       curves of  the system




       Hence,  corresponding  to  given  initial  values,  there  is  a  unique  auto-
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