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76          11.  TOPOLOGY  OF  DIFFERENTIABLE  MANIFOLDS





        and therefore, by the completeness of  the system of  subspaces AP,(T*),
        A$(TT) and  A&(T*) in  AD(T*), a; = ad, a;  = a,,  a;  = a~. We  have
        proved:
          A regular form  a of  degree p  may be  uniquely decomposed into the sum


        where ad E A$(T*),  a,  E  A$(T*) and  a~ E  API(T*).
          This is the Hodge-de Rham  decomposition theorem [39].


                          2.1 1.  Fundamental theorem

          At  this  stage  it  is  appropriate  to state  the existence theorems of  &
        Rham  [65]-the   proofs  of  which  appear in Appendix A.
                       (i
          (R,) Let  {q} = 1,  ***,  b,(M))  be  a  base  for  the (rational) p-cych
        of  a  compact  dz#eeentiable  manifold  M  and  wk  (i = 1,   ., b,(M))  be  bp
        arbitrary  real constants.  Then, there exists a  regular, closed p-form  a on
        M  having  the  wk  ar periods,  that is




          (R,) A closed form  having zero perrbdc  is an exact form.
          We  now  establish the  existence theorem  due to  Hodge  which  is  at
        the very foundation of  the subject matter  of  curvature  and homology.
          There  exists  a  unique  harmonic form  a of  degrree p  having  arbitrarily
        assigned periods  on  bp independent p-cycles  of  a  compact  and  orientable
        Riemannian  manifold.
          Indeed,  let  a  be  a  closed  p-form  having  the  given  periods.  The
        existence of  a is  assured by  the  first of  de  Rham's  theorems.  By  the
        decomposition theorem  a = ad + am  (Since or  is closed, a,  is zero and
        consequently a is orthogonal to  A$(T*)). Since ord  E  A$(Tt) its periods
        are  zero.  Hence  the  periods  of  a,  are  those  of  a. The  uniqueness
        follows from  (R,)  since a  harmonic form  whose  periods vanish is the
        zero form.
          Let  M be  a  compact  and  orientable  Riemannian  manifold.  Then,  the
       number of  linearly independent real harmonic forms  of  degrec p is equal to the
        pth betti number  of  M.
          For, let vd denote the harmonic p-form whose periods are zero except
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