Flexible wavelet transforms using lifting
Author(s) -
Roger L. Claypoole,
Richard G. Baraniuk
Publication year - 1998
Publication title -
rice digital scholarship archive (rice university)
Language(s) - English
Resource type - Conference proceedings
DOI - 10.1190/1.1820329
Subject(s) - wavelet , computer science , wavelet transform , haar wavelet , haar , lifting scheme , signal processing , noise reduction , computer graphics (images) , artificial intelligence , discrete wavelet transform , digital signal processing , computer hardware
Roger L. Claypoole, Jr. and Richard G. Baraniuk, Rice University Summary We introduce and discuss biorthogonal wavelet transforms using the lifting construction. The lifting construction exploits a spatial{domain, prediction{error interpretation of the wavelet transform and provides a powerful framework for designing customized transforms. We discuss the application of lifting to adaptive and non{linear transforms, transforms of non{uniformly sampled data, and related issues. Introduction Many applications (compression, analysis, denoising, etc.) bene t from signal representation with as few coe cients as possible. We also wish to characterize a signal as a series of course approximations, with sets of ner and ner details. The Discrete Wavelet Transform (DWT) provides such a representation. The DWT represents a real-valued discrete-time signal in terms of shifts and dilations of a lowpass scaling function and a bandpass wavelet function [2]. The DWT decomposition is multiscale: it consists of a set of scaling coe cients c0[n], which represent coarse signal information at scale j = 0, and a set of wavelet coe cients dj [n], which represent detail information at scales j = 1; 2; : : : ; J . The forward DWT has an e cient implementation in terms of a recursive multirate lterbank based around a lowpass lter h and highpass lter g [12, pp. 302{332]. The inverse DWT employs an inverse lterbank with lowpass lter eh and highpass lter eg, as shown in Figure 1 For special choices of h, g, eh, and eg, the underlying wavelet and scaling functions form a biorthogonal wavelet basis [2].
Accelerating Research
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom
Address
John Eccles HouseRobert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom