Page 233 - Curvature and Homology
P. 233

6.7.  Zero  curvature

          In this section we examine the effect of zero curvature on the properties
        of  hermitian  manifolds-the   curvature being defined as in  5 5.3.

        Theorem 6.7.1.   The curvature of  an hermitian manifold.vanishes, if and
        only  if, it is possible  to choose a parallel  field  of  orthonormal holomorphic
       frames  in a  naghborhood of  each point  of  the manifold.
          By  a field  of frames  on  the manifold  M or  an  open subset  S of  M
        is meant a cross section in the (principal) bundle of frames over M or S,
        respectively.  The field is said to be parallel  if  each of  the vector fields
        is  parallel.
          We first prove the sufficiency. If the curvature is zero, the system of
        equations  w5,  = 0  is  completely  integrable.  Therefore,  in  a  suitably
        chosen  coordinate  neighborhood  U  of  each  point  P it  is  possible  to
        introduce  a field of  orthonormal  frames P, (el, .--, e,,  ll, --.,  which
        are parallel and  are uniquely determined  by  the initially chosen frame
        at P.  For, by  5  1.9 the vector fields e,  satisfy the differential system

                                 de, = di e,.
        (The metric  being locally flat, the e,  may  be thought of  as covectors.)
        Of  course,  we  also  have  the  conjugate  relations.  Since  the  e,  are  of
        bidegree  (l,O),  the  condition  &,  = 0  implies  d"e,  = 0, that  is  the  e,
        are holomorphic vector fields. Hence, the condition that the curvature
        is  zero  implies the  existence  of  a  field  of  parallel  orthonormal  holo-
        morphic frames in  U.
          Conversely, with respect to any parallel field of  orthonormal  frames
       the equations



       imply  Rjikl, = 0.  The curvature  tensor  must  therefore  vanish  for  all
        frames.
          Let us call the neighborhoods U of  the theorem admissible neighbor-
        hoods. Parallel displacement of  a frame at P along any path in such  a
        neighborhood  IJ  of  P is  independent  of  the  path  since  the  system
        wij = 0  has  a  unique  solution  through  U  coinciding with  the  given
        frame at P E U.  (In the remainder  of  this section we  shall write  U(P)
        in place of  U).
          Now,  given  any two points Po and PI of  the manifold and a path  C
       joining  them,  there  is  a  neighborhood  U(C) = U U(Q)  of  C  such
                                                   QEC
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