Page 92 - Curvature and Homology
P. 92

74         11.  TOPOLOGY  OF  DIFFERENTIABLE  MANIFOLDS

        from which


        By  (2.8.7),  this may also be written as


          Two linear operators A and A' are said to be dual if (Aa, p) = (a, A'p)
        for  every pair of forms a and p for which both sides of the relation are
        defined.  Thus, the operators  d  and 8 are dual.
          In the same way,  we see that, if  /3  is of  degree p - 1, then


        Hence, in  order  that  a be  closed,  it is necessary  and sufient  that it be
        orthogonal to all co-exact forms  of  degree p.
          The condition  is indeed necessary; for,  if  da = 0, then  (a, Sp) = 0
        for  any  (p + 1)-form p.  Suppose  that  a  is  orthogonal  to  all  co-exact
        forms  of  degree p.  Then,  (a, Sda) = 0,  and  so  (da,  da) = 0.  Hence,
        from property (i), p. 71, it follows that da = 0.
          In order that a form  be  co-closed,  it is necessary and sujickt  that it be
        orthogonal to all exact forms.  It follows that if  ar and p are two p-forms,
        a being exact and  co-exact, then (a, 8) = 0.
          We now  show that in  a  compact  Riemannian  manifold the defznitions
        of  a  harmonic form  given by  Hodge and Kodaira  are equivalent.  Assume
        that a is a harmonic form in the sense of  Kodaira.  Then,


        Hence,  since (da, da) 2 0 and (Sa,  Sa) 2 0,  it follows that da = 0 and
        Sa = 0.  The converse is trivial.
          In particular, a  harmonic function  in a compact Riemannian manifold is
        necessarily a  constant.
          We have seen that a harmonic form on a compact manifold is closed.
        This statement is false if the manifold is not compact. For, a closed form
        of  degree 0 is a constant while in En there certainly exist non-constant
        harmonic functions.
          The differential forms of degree p form a linear space AP(T*) over R.
        Denote  by  AP,(T*),  A$(T*)  and  AMT*)  the  subspaces  of  AP(T*)
        consisting  of  those  forms  which  are  exact,  co-exact  and  harmonic,
        respectively.  Evidently,  these subspaces are orthogonal in  pairs,  that is
        forms  belonging  to  distinct  subspaces  are  orthogonal.  A  prform
        orthogonal to the three subspaces is necessarily zero (cf. 5 2.10). In other
        words,  the  subspaces  A,P(T*),  Ai(T*)  and  AL(T*)  form  a  complete
        system in  AP(T*).  (We have previously written  A,P(T*) for  AZ(T*)).
   87   88   89   90   91   92   93   94   95   96   97