Page 120 - Curvature and Homology
P. 120

1 02    111.  RIEMANNIAN MANIFOLDS:  CURVATURE, HOMOLOGY
        On the other hand, by conditions (ii) and (iii), 8(X) may be extended to
        all  of  A(T).  In fact,  O(X)  may  be  extended  to the  tensor  algebras of
        contravariant and covariant tensors by insisting that (for each X) it be a
        derivation of  these  algebras.  For example, by  lemma 3.4.3
                                        Y - 9t.Y
                             4X)Y = lim
                                     t*     t
        where  q~, is  the  1-parameter  group  generated  by  X.  Hence, for  any
        tensor t of  type (p, 0)
                                        t -  t
                                           9:.
                             B(X) t = lim
                                    s-r6   S
        where  q~:,   =   @   @ vs. (p times) is the induced  map in  T:.   (For
        any  XI, -, X,  E T, &(XI  @ *.. @ Xp) = (pl.(X1)  @   @ va.(Xg)).
          Since [8(X), 8(Y)]  = 8(X) 8(Y) - B(Y) 8(X) is a derivation, it follows
        from the Jacobi  identity that the  map  x L.B(X) is  a  representation
        of  the Lie algebra of  tangent vector fields.


        Lemma 3.5.1.   The  derivations  d, i(X),  and  B(X)  are  dated by  the
        formula
                             B(X) = i(X)d + di(X).              (3.5.1)

          Since both  sides are derivations, and since the Grassman algebra of
        differential forms is generated by its homogeneous elements of  degrees
        0 and  1, the relation need only be established for differential forms of
        degrees 0 and  1 :





        Lemma 3.5.2.   For  a  I-form  u on  M  and any  tangent  vector jieldr  X
        and Y on M :
                    <X A Y, da)  = Xar(Y) - Yar(X) - a([X,Y]).   (3.5.2)
          The right  hand  side  is  meaningful since at each point  P of  M, Tp
        and  T,* are dual vector spaces. Thus, u is a linear map from  T into F.
        By  linearity,  it  is  sufficient  to  prove  the  relation  for  X  = a/ihi,
        Y = a/au* and  u = gdf where f and g are  functions  expressed in the
        coordinates (3). In fact, if the relation holds for a, j3  E A1(T*), it holds
        for u + /3  and fa where f is a differentiable function. We may therefore
        assume u = duk and in this case, both sides vanish.
   115   116   117   118   119   120   121   122   123   124   125