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The reflection principle, the Schwarz potential and quadrature.

机译:反射原理,Schwarz势和正交。

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摘要

The Schwarz reflection principle for harmonic functions in R 2 can be stated as follows. Let Gamma ⊂ R 2 be a non-singular real analytic curve and P ' ∈ Gamma. Then, there exists a neighborhood U of P' and an anticonformal mapping R : U → U which is identity on Gamma, permutes the components U 1, U2 of UGamma and relative to which any harmonic function u(x,y) defined near Gamma and vanishing on Gamma satisfies the reflection law u(x0, y0) = -u( R(x0, y0)) for any point (x0,y0) sufficiently close to Gamma, where the mapping R is given by R(x0,y0) = R(z0) = Sz0 , and S is the Schwarz function of the curve Gamma.;In Chapter 2, a more general point-to-point reflection law of the form u(P) = a≤ N calphaDalpha u(Q), where N, c alpha ( a ≤ N) are constants depending only on P and Q, is investigated for the solutions of the more general Helmholtz equation in two independent variables, and partial negative answers to the point to compact set reflection conjecture suggested by Garabedian and others are obtained.;In Chapter 3, a reflection formula for polyharmonic functions in R2 is obtained. The formula generalizes the celebrated Schwarz reflection principle for harmonic functions to polyharmonic functions. Modification of the obtained formula to the case of nonhomogeneous data on a reflecting curve is also discussed.;A natural generalization of the Schwarz function to higher dimensions is called the Schwarz potential or the modified Schwarz potential of the surface.;In an effort to prove "the Schwarz potential conjecture" and to study quadrature for harmonic functions, the Schwarz potential of the first few nontrivial surfaces (spheres, cylinders, cones and ellipsoids) has been studied by Khavinson and Shapiro.;In the last Chapter 4, a method to explicitly calculate the modified Schwarz potential and the corresponding quadrature distribution of axially symmetric solid tori in even dimensional spaces is suggested. The quadrature formula for functions harmonic inside the torus and integrable over the torus is also established and examples are provided.
机译:R 2中谐波函数的Schwarz反射原理可以描述如下。令R 2为非奇异实数分析曲线,P'∈Gamma。然后,存在P'的邻域U和反保形映射R:U→U,它在Gamma上是恒等的,置换UGamma的分量U 1,U2,相对于在Gamma附近定义的任何谐波函数u(x,y)并且在Gamma上消失就足以满足足够接近Gamma的任何点(x0,y0)的反射定律u(x0,y0)= -u(R(x0,y0)),其中映射R由R(x0,y0 )= R(z0)= Sz0,并且S是曲线Gamma的Schwarz函数。;在第二章中,形式更普通的点对点反射定律u(P)=a≤N calphaDalpha u(Q ),其中N,c alpha(a≤N)是仅取决于P和Q的常数,研究了更一般的Helmholtz方程在两个独立变量中的解决方案,并提出了关于紧定集合反射猜想的部分否定答案在第三章中,得到了R2中多调和函数的反射公式。该公式将著名的Schwarz反射原理从谐波函数推广到多谐波函数。还讨论了将获得的公式修改为反射曲线上不均匀数据的情况。将Schwarz函数自然推广到更高维度的过程称为Schwarz势或表面的修改Schwarz势。 Khavinson和Shapiro研究了“ Schwarz势猜想”并研究谐波函数的正交,对前几个非平凡表面(球,圆柱,圆锥和椭球)的Schwarz势进行了研究;在最后的第4章中,明确地计算出修正的Schwarz势,并建议在偶数维空间中轴对称固体托里的相应正交分布。还建立了函数在圆环内部和在圆环上可积分的正交公式,并提供了示例。

著录项

  • 作者

    Aberra, Dawit Wakjira.;

  • 作者单位

    University of Arkansas.;

  • 授予单位 University of Arkansas.;
  • 学科 Mathematics.
  • 学位 Ph.D.
  • 年度 2000
  • 页码 53 p.
  • 总页数 53
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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