首页> 外文学位 >Random variable dilation equations in R(d) and the stability of scaling functions.
【24h】

Random variable dilation equations in R(d) and the stability of scaling functions.

机译:R(d)中的随机变量膨胀方程和缩放函数的稳定性。

获取原文
获取原文并翻译 | 示例

摘要

Let Γ be a lattice in Rd and let M be an expansive matrix, meaning all eigenvalues have moduli greater than 1, such that MGG . A dilation equation has the form 4x=SgGag 4Mx+g, where a:= ag gG is in l1 (Γ). A function which solves a dilation equation is known as a scaling function. If an L2-solution to this equation exists, it may be used to generate multiresolution analyses and wavelet bases, which are powerful tools in signal and image processing [4], [19], [20]. Other applications of scaling functions include interpolating subdivision schemes for computer-aided design [5], [3]. If a∈l2 (Γ) then the dilation equation will have a compactly supported solution, which may be a distribution [7], [4]. The problem of finding a solution which is a function can be recast in terms of probability: suppose G1, G2, …are i.i.d. random variables on a probability space W,F,P and suppose Z: =k=1>∞M-k Gk is finite. Then Z is a solution to a random variable dilation equation MZ=dZ+G, where Z and G are independent and G=dG1. Gundy [11] has shown that £ (Z) is absolutely continuous if and only if the fractional part of Z is uniform for the one-dimensional case. In this thesis we generalize Gundy's result to higher dimensions under the assumption that G has values in a finite subset of the lattice and prove a sufficient condition on the distribution of G to obtain a solution which has a density function. The techniques used to achieve these results reflect the increased complexity of the problem in higher dimensions, which is due primarily to the fact that M may produce a rotation as well as a dilation, and may even be non-normal. We also present an improved version of an algorithm described by Lawton, Lee and Shen [16] for determining the stability of the scaling function.
机译:令Γ为 R d 中的晶格,令 M 为扩展矩阵,这意味着所有特征值均具有更大的模量小于1,这样 M G G 膨胀方程的格式为 4 x = < g> S g G a g 4 Mx + g 其中 a := a g g G 位于 l 1 (Γ)中。解决膨胀方程的函数称为缩放函数。如果该方程的 L 2 解存在,则可以用于生成多分辨率分析和小波基,这是信号和图像处理的强大工具[4], [19],[20]。缩放功能的其他应用包括用于计算机辅助设计的内插细分方案[5],[3]。如果 a∈l 2 (Γ),则扩张方程将具有紧致支持的解,该解可能是分布[7],[ 4]。可以用概率来重现找到作为函数的解的问题:假设 G 1 G 2 ,…是我概率空间上的随机变量 W F, P 并假设 Z = k = 1 >∞ M -k G k math>是有限的。那么 Z 是随机变量膨胀方程 MZ = d Z + G, 的解,其中 Z G 是独立的, G = d G 1 Gundy [11]表明,当且仅当一维情况下 Z 的小数部分一致时,£( Z )是绝对连续的。在本文中,我们假设 G 在晶格的有限子集中具有值,并假设在 G 的分布上有充分的条件以获得具有密度函数的解决方案。用于获得这些结果的技术反映了问题在更高维度上的日益复杂性,这主要是由于 M 可能会产生旋转以及扩张,甚至可能是非扩张性的。正常。我们还介绍了Lawton,Lee和Shen [16]描述的用于确定缩放函数稳定性的算法的改进版本。

著录项

  • 作者

    Belock, Julie Anne.;

  • 作者单位

    Lehigh University.;

  • 授予单位 Lehigh University.;
  • 学科 Mathematics.
  • 学位 Ph.D.
  • 年度 1999
  • 页码 74 p.
  • 总页数 74
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 数学;
  • 关键词

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号