Page 48 - Curvature and Homology
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30                 I.  RIEMANNIAN MANIFOLDS

        space T, at x E B onto the tangent  space T,.,. This, in turn gives rise
        to an isomorphism of  T:., onto  T,*.  On the other  hand, the projection
        map w  induces a map T* of  T:  (the space of  covectors at P E M). An
        affine connection on M may  then be described as follows:
          (i)  T,* is the  direct  sum  of  W,* and w*(T,*) where  Wz is  a  linear
        subspace at  x E B and  n(x) = P;
                                                                   by
          (ii)  For  every a  E GL(n, R) and x E B,   is the image of  c.,
        the induced map on the space of  covectors.
          In other words, an aflne connection on M  is a choice of  a subspace W*,
        in  T,*  at each point  x of  B subject to the conditions (2')  and (it]. Note that
        the dimension of  W,* is n2. Hence, it can be defined by  prescribing n2
        linearly  independent  differential  forms  which  together  with  the  85
        span  Tz.


                           1.9.  Riemannian geometry
          Unless otherwise indicated, we shall assume in the sequel that we are
        given a differentiable manifold M  of  dimension n and class 00.
          A Riemannian metric on M is a tensor field g of type (0,2) on M subject
        to the conditions:
          (i) g is a symmetric tensor  field, and
          (ii) g is positive definite.
        This tensor field is called the  fundamental  tensor field. When a Riemannian
        metric  is  given  on  M the  manifold  is  called  a  Riemannian  manifold.
        Geometry  based  upon  a  Riemannian  metric  is  called  Riemannian
        geometry.  A  Riemannian metric gives rise to an inner (scalar) product
        on  each tangent  space  Tp at P E M:  the scalar product  of  the contra-
        variant  vector  fields  X = 64(a/hc) and  Y = qi(a/aui)  at the  point  P
        is defined to be the scalar





        The positive square root of  X  X is called the length of  the vector X.
        Since the  Riemannian metric is a tensor field, the quadratic differential
        form
                                d.@  = gjk duj duk              (1 .9.2)
        (where we  have written  duj duk  in place of  duj  @ duk for convenience)
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