Page 30 - Curvature and Homology
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12                 I.  RIEMANNIAN MANIFOLDS

        symmetric tensor field  called the curl of  the vector 6,.  If  the 6,  define
        a gradient  vector field, that  is,  if  there exists a real-valued  function f
        defined on an open subset of  M  such that 6,  = (af/dui),  the curl must
        vanish.  Conversely, if  the curl of  a (covariant) vector field vanishes, the
        vector  field is  necessarily  a (local) gradient  field.



                             1.4.  Differential forms
          Let M be a differentiable manifold of  dimension n. Associated to each
        point P E M, there is the dual space Tp* of  the tangent  space Tp at P.
        We have seen that T$ can be identified with the space of linear differential
        forms  at P.  Hence,  to  a  1-dimensional subspace  of  the tangent  space
        there  corresponds  a linear  differential form.  We  proceed to show that
        to  a  p-dimensional  subspace  of  Tp corresponds  a  skew-symmetric
        covariant tensor of  type (0, p), in fact, a 'differential form of  degree P'.
        To this end, we  construct  an  algebra over  Tp* called the  Grassman or
        exterior  algebra:
          An  associative  algebra  A (V)  (with  addition  denoted  by  + and
        multiplication  by  A)  over  R  containing  the  vector  space  V  over  R
        is called a Grassman or exterior algebra if
          (i)  A (V) contains the unit  element  1 of  R,
          (ii)  A (V) is generated by  1 and the elements of  V,
          (iii)  If x E V,  x  A x = 0,
          (iv)  The dimension of  A (V) (as a vector space) is 2n,  n =dim  V.
          Property  (ii) means that  any  element  of  A (V) can  be  written  as a
        linear combination of  1 E R  and of  products of  elements of  V,  that is
        A (V) is generated from V and 1 by the three operations of the algebra.
        Property  (iii)  implies  that  x  A y = - y  A x  for  any  two  elements
        x,  y E V.  Select  any  basis (el, ..., en}  of  V.  Then,  A (V)  contains  all
        products  of  the  e,  (i = 1, ..., n).  By  using  the  rules



        we  can arrange any product  of  the e,  so that it is of  the form




        or else, zero.  The latter  case arises when the original product  contains
        a repeated  factor. It follows that we  can compute any product  of  two
        or  more vectors alel + ... + anen of  V as a linear  combination  of  the
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