三元正交小波的构造

高维小波分析是分析和处理多维数字信号的有力工具.张量积小波有其自身的缺点.本文给出构造紧支撑三元不可分正交尺度函数和正交小波函数的新算法.当尺度函数的符号中含有因子1 z1221 z2221 z322的幂指数越高时,尺度函数越光滑.     

小波紧框架的显式构造

该文研究对应于3带尺度函数的小波紧框架,这个小波紧框架是由V_1中的l个函数ψ^1, ψ^2, ψ^n 构成.给出这l个函数构成小波紧框架的充分条件.由此给出由3 带尺度函数构造出一个小波紧框架的显式公式.特别的,如果给定尺度函数的符号是有理函数,则可以构造出符号为有理函数的小波紧框架.最后还给出类似于小波的小波紧框架的分解与重构算法.      

小波紧框架的构造

小波框架理论是小波分析的重要内容之一.本文对于4-带尺度函数,由V1中的l个函数ψ1,ψ2,…,ψl构造小波紧框架.首先给出这个l个函数构成小波紧框架的充分条件.由此给出由4-带尺度函数构造出一个小波紧框架的公式.最后还给出类似于小波的小波紧框架的分解与重构算法.     

关于Lnn√z与1/nLnz是否相等的讨论

对复变量2的函数Lnn√z与1/nLnz的关系进行研究，发现Lnn√z与1/nLnz，并给出证明，纠正Lnn√z与1/nLnz是两个不同函数”的错误认识．     

正交多小波的构造

1 引言 在小波的构造和应用中,对于2尺度单一小波已有相当成熟的理论,特别是在小波构造方面,若知道正交单一尺度函数,相应的单一小波是很容易构造出的。对于a尺度紧支撑多小波,如何从已知的a尺度紧支撑多重尺度函数构造出相应的多小波,到目前为止尚没有一般的构造方法。W.Lanton等用仿酉矩阵扩充的方法构造出相应的多小     

a尺度正交多尺度函数和正交多小波

基于a 尺度正交单尺度函数，分别给出重数为2和3的a 尺度正交多尺度函数的构造算法。并给出对应正交多小波的显式构造。最后给出伸缩因子为3的正交多小波的构造算例。     

M带紧支撑正交对称复尺度函数的构造

1 引言 近年来,小波的研究主要集中于实值小波,并得到了许多优美的结果。如Daubechies构造一系列2带正交小波,Chui和Lian构造若干3带既正交又对称的尺度函数和小波,杨守志,程正兴等,构造出既正交又对称的4带尺度函数和小波,对M≥3这样的一般情形,Bi,Dai和Sun给出M带正交的Daubechies类尺度函数的通用滤波器表     

α带小波紧框架的显式构造方法

文中研究了对应于α-带尺度函数的小波紧框架,这个小波紧框架是由V₁中的n个函数ψ¹,ψ²,...,ψⁿ构成. 首先给出了这n个函数构成小波紧框架的充分条件, 并借助尺度函数给出了构造小波紧框架的显式公式. 如果尺度函数的符号是有理函数,则可以构造出符号为有理函数的小波紧框架. 其次给出类似于正交小波的小波紧框架的分解与重构算法,并构造了小波紧框架的数值算例.     

小波变换及其应用(续三)

两维正交小波基　在许多实际问题中 ,经常会遇到多维的信号 (如图像等 ) ,因此只有一维小波基是不够的。不难证明 (见 [1 ])若φ( t)与Ψ ( t)是小波标准正交基的尺度函数与母函数 ,φjm( x) =2 j2 φ( 2 jx -m) ,Ψjm( x) =2 j2 Ψ ( 2 jx -m) ,则 {Ψjn( x)φjm( y) ,φjn( x)Ψjm( y) ,Ψjn( x)Ψjm( y) }j,m,nz构成两维平方可积函数空间 (即满足∫∞-∞∫∞-∞|f ( x,y) |2 dxdy <∞的全体函数所构成的线性空间 )的一组标准正交基 (见图 1 2 ( a) ( b) )图 1 2(六 )离散小波变换的应用举例( 1 )消除信号中的噪音信号在生成和传输过程…     

函数方程组的亚纯解(英文)

本文主要研究以下类型函数方程组亚纯解的存在性和增长性问题{f1n（cz）=a（z） (f₁^m1（z）/(f₂^m2（z）),f₂ n（cz）=b（z）(f₂（m1）^z)/(f₁^m2（z）),其中a（z）,b（z）为有理函数,|c|=0,1,n>1,mi>1（i=1,2）.利用亚纯函数的Nevanlinna值分布理论与及复函数方程研究部分方法,获得了定理1,2,3三个关于函数方程组的结果,推广了函数方程中的一些结果.     

Smoothing Minimally Supported Frequency Wavelets: Part II

The main purpose of this paper is to give a procedure to "mollify" the low-pass filters of a large number of Minimally Supported Frequency (MSF) wavelets so that the smoother functions obtained in this way are also low-pass filters for an MRA. Hence, we are able to approximate (in the L²-norm) MSF wavelets by wavelets with any desired degree of smoothness on the Fourier transform side. Although the MSF wavelets we consider are bandlimited, this may not be true for their smooth approximations. This phenomena is related to the invariant cycles under the transformation $x\mapsto 2x (\mbox{mod}2\pi).The main purpose of this paper is to give a procedure to “mollify” the low-pass filters of a large number ofMinimally Supported Frequency (MSF) wavelets so that the smoother functions obtained in this way are also low-pass filters for an MRA. Hence, we are able to approximate (in the L ² -norm) MSF wavelets by wavelets with any desired degree of smoothness on the Fourier transform side. Although the MSF wavelets we consider are bandlimited, this may not be true for their smooth approximations. This phenomena is related to the invariant cycles under the transformation x ?2x (mod2π). We also give a characterization of all low-pass filters for MSF wavelets. Throughout the paper new and interesting examples of wavelets are described.     

Smoothing minimally supported frequency wavelets: Part II

The main purpose of this paper is to give a procedure to “mollify” the low-pass filters of a large number ofMinimally Supported Frequency (MSF) wavelets so that the smoother functions obtained in this way are also low-pass filters for an MRA. Hence, we are able to approximate (in the L ² -norm) MSF wavelets by wavelets with any desired degree of smoothness on the Fourier transform side. Although the MSF wavelets we consider are bandlimited, this may not be true for their smooth approximations. This phenomena is related to the invariant cycles under the transformation x ↦2x (mod2π). We also give a characterization of all low-pass filters for MSF wavelets. Throughout the paper new and interesting examples of wavelets are described.     

Stability and Independence for Multivariate Refinable Distributions

Due to their so-called time-frequency localization properties, wavelets have become a powerful tool in signal analysis and image processing. Typical constructions of wavelets depend on the stability of the shifts of an underlying refinable function. In this paper, we derive necessary and sufficient conditions for the stability of the shifts of certain compactly supported refinable functions. These conditions are in terms of the zeros of the refinement mask. Our results are actually applicable to more general distributions which are not of function type, if we generalize the notion of stability appropriately. We also provide a similar characterization of the (global) linear independence of the shifts. We present several examples illustrating our results, as well as one example in which known results on box splines are derived using the theorems of this paper.     

联系Butterworth滤波器的双正交小波

联系Butterworth滤波器的双正交小波称为Butterworth小波,它们具有很好的性质:包括对称性,插值性及消失矩．本文定义了离散空间L~2(Z)中的双正交小波并给出一个易于验证的充分条件．利用这一条件,重新得到Butterworth小波;进一步,构造了一类双正交小波．它们不仅具有Butterworth小波的前述所有性质,而且具有最短可能的支集．     

REAL-VALUED PERIODIC WAVELETS: CONSTRUCTION ANDRELATION WITH FOURIER SERIES

1.IntroductionWaveletshaverecentlyreceivedagreatdealofattentioninsuchareasassignalprocessingandimageprocessing([12],[8]).Variousmethodstoconstructwaveletshavebeengiven([14],[13],[9],[7]).Itiswellknownthatinmathematicsandmathematicphysicsmanyperiodicp...     

小波连通性研究进展

本文介绍了L²(R)中一些特殊小波组成集在L²(R)中的拓扑几何性质——道路连通性,特别综述了近二十年来小波连通问题研究的主要进展并列出了一些悬而未决的问题,并简要说明了高维情形和其他情形的相应结果.     

State Analysis and Optimal Control of Time-Varying Discrete Systems via Haar Wavelets

The state analysis and optimal control of time-varying discrete systems via Haar wavelets are the main tasks of this paper. First, we introduce the definition of discrete Haar wavelets. Then, a comparison between Haar wavelets and other orthogonal functions is given. Based upon some useful properties of the Haar wavelets, a special product matrix and a related coefficient matrix are proposed; also, a shift matrix and a summation matrix are derived. These matrices are very effective in solving our problems. The local property of the Haar wavelets is applied to shorten the calculation procedures.     

Isometries, shifts, Cuntz algebras and multiresolution wavelet analysis of scaleN

In this paper we show how wavelets originating from multiresolution analysis of scaleN give rise to certain representations of the Cuntz algebrasO _N , and conversely how the wavelets can be recovered from these representations. The representations are given on the Hilbert space by (S _i ) (z)=m _i (z)(z ^N ). We characterize the Wold decomposition of such operators. If the operators come from wavelets they are shifts, and this can be used to realize the representation on a certain Hardy space over . This is used to compare the usual scale-2 theory of wavelets with the scale-N theory. Also some other representations ofO _N of the above form called diagonal representations are characterized and classified up to unitary equivalence by a homological invariant.Work supproted in part by the U.S. National Science Foundation and the Norwegian Research Council.     

紧支撑正交对称和反对称小波的构造

１．引言 近年来,人们分别从数学和信号的观点对正交小波进行了广泛的研究．尤其是２尺度小波,它克服了短时 Ｆｏｕｒｉｅｒ变换的一些缺陷．目前最常用的 ２尺度小波是 Ｄａｕｂｅｃｈｉｅｓ 小波,但 ２尺度小波也存在一些问题：如 Ｄａｕｂｅｃｈｉｅｓ［２］已证明了除 Ｈａａｒ小波外不存在既正交又对称的紧支撑 ２尺度小波．因此人们提出了 ａ尺度小波理论［３］－［６］,文献［４］－［６］对 ４尺度小波迸行研究．本文的目的是研究４尺度因子时紧支撑正交对称和反对称小波的构造方法．并指出对同一紧支撑正交对称尺度函数而言,…