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  • articleNo Access

    On the growth of von Neumann dimension of harmonic spaces of semipositive line bundles over covering manifolds

    We study the harmonic space of line bundle valued forms over a covering manifold with a discrete group action, and obtain an asymptotic estimate for the von Neumann dimension of the space of harmonic (n,q)-forms with values in high tensor powers of a semipositive line bundle. In particular, we estimate the von Neumann dimension of the corresponding reduced L2-Dolbeault cohomology group. The main tool is a local estimate of the pointwise norm of harmonic forms with values in semipositive line bundles over Hermitian manifolds.

  • chapterNo Access

    BERGMAN FUNCTION AND DIRICHLET PROBLEM IN CLIFFORD ANALYSIS

    In this paper, we generalize the results of1, on theory of hyperholomorphic analysis to the case for several variables, that is, Clifford analysis. These results are not only of theoretical importance but also parctical interest. In fact, we also generalize3, the Dirac operator formula to formula. When the base i ={i1, …,in} is given, the Dirac operator D is determined, while ψD may consider as the rotation transform on the vector ψ = {ψ1, … , ψn}. Such a generalization is similar to Descartes coordinate system to the moving coordinate system, therefore, it is very convenient to build some basic formulas on Clifford analysis and to find some analytic representations of differential equations. From this idea, we obtain a very important representation of Bergman kernel function:

    this is a key formula for proving Bergman kernel function ψB to be a projector of Lp(Ω,C(Vn,0)) onto ψAp(Ω,C(Vn,0)), where φ,ψC is a compact operator. Moreover, we build up some results on Clifford analysis, such as Stokes formula, Borel-Pompeiu formula and Cauchy formula, propreties of Bergman kernel function. Moreover as their application, we discuss the Dirichlet problem for related bi-analytic functions of several variables on the bounded simply-connected domain with smooth boundary, and then representations of solution are obtained.