Page 17 - Curvature and Homology
P. 17

INTRODUCTION                     xvii

        geometry, in particular,  Kaehler  geometry along the lines  proposed by
        S.  Chern.  Its influence  on  the  homology structure of  the  manifold  is
        discussed  in  Chapters  V  and  VI.  Whereas  the  homology  properties
        described  in  Chapter  I11  ar8 similar  to  those  of  the  ordinary  sphere
        (insofar  as betti  numbers are concerned),  the corresponding  properties
        in Chapter VI are possessed by P, itself. Families of  hermitian manifolds
        are  described, each  including P, and retaining  its  betti  numbers.  One
        of the most important applications of the effect of curvature on homology
        is to be found  in the vanishing  theorems due to K.  Kodaira.  They are
        essential in the applications  of  sheaf theory to complex manifolds.
          A conformal transformation of  a compact  Riemann surface is a holo-
        morphic  homeomorphism.  For  compact  Kaehler  manifolds  of  higher
        dimension,  an element of  the  connected  component  of  the identity  of
        the group of conformal transformations is an isometry, and consequently
        a holomorphic homeomorphism.  More  generally,  an infinitesimal con-
        formal map  of  a compact  Riemannian  manifold  admitting a harmonic
        form of  constant length is an infinitesimal  isometry. Thus, if  a compact
        homogeneous  Riemannian  manifold  admits  an  infinitesimal  non-iso-
        metric conformal transformation,  it is a homology sphere. Indeed, it is
        then  isometric  with  a  sphere.  The conformal transformation  group  is
        studied in  Chapter 111, and in  Chapter VII groups of  holomorphic as
        well  as  conformal  homeomorphisms  of  Kaehler  manifolds  are  in-
        vestigated.
          In Appendix A, a proof of  de Rham's theorems based on the concept
        of  a sheaf  is given although this notion is not defined.  Indeed, the proof
        is but an adaptation from the general theory of sheaves and a knowledge
        of  the subject is not required.
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