Page 29 - Curvature and Homology
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1.3.  TENSOR BUNDLES                 11
        structure  derived  from  the  Euclidean  space of  the  components  of  its
        elements  it  becomes  a  differentiable  manifold.  Now,  a  topology  is
        defined in 9-1 by  the requirement  that for each  U, qu maps open sets
        of  U x  T: into  open  sets of  F:. In this  way, it can be shown that Fi
        is  a separable  Hausdorff  space. In fact, .Ti is  a  differentiable  manifold
        of  class k - 1 as one sees from the equations (1.3.7).
          The  map  gUv: U  n V -t GL(c) is  continuous  since  M is of  class
        k 5 1. Let P be a point in the overlap of  the three coordinate neighbor-
        hoods,  U,V,W  U n V  n W # 0. Then,

        and since



        these  maps  form  a  topological  subgroup  of  GL(T~. The  family  of
        maps guv for  U n V # $. where  U,  V, ... is a covering of  M is called
       the set of  transition functions  corresponding  to the given  covering.
          Now, let
                                 m:q-+M

        be  the  projection  map  defined  by ?r(c(P)) = P.  For  1 < k,  a  map
                 of
       f: M -+ c class  1 satisfying n  f = identity is called a tensor field of
       type (r, s) and class 1.  In particular, a tensor field of  type (1,O) is called
        a vector field or an injinitesimal transformation.  The manifold 9-i is called
       the tensor bundle over the base space M with structural group GL (nr+8, R)
        and j3re c. In the general theory of  fibre bundles, the map f is called
        a  cross-section.  Hence, a  tensor field of  type  (r, s)  and  class  1 < k  is  a
        cross-section of  class 1 in the tensor  bundle c over  M.
         The bundle     is usually  called the tangent bundle.
         Since  a  tensor field  is  an  assignment  of  a  tensor  over  Tp for each
        point  P E M,  the  components - af/aur  (i = 1, ..., n)  in  (1.2.8)  define  a
        covariant  vector  field  (that  is,  there  is  a  local  cross-section)  called
        the gradient  off.  We may ask  whether  differentiation  of  vector  fields
        gives  rise  to  tensor fields, that  is  given a  covariant  vector field ti, for
        example (the ti are the components of a tensor field of  type  (O,l)),  do
        the n2 functions  agt/auj define  a tensor  field (of type (0,2)) over' U? We
        see from (1.2.12)  that the presence of the term (a2uj/atikari3fj in




       yields a negative  reply.  However, because of  the symmetry  of  i and k
       in the second term on the right the components +jrk - +jkt  define a skew-
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