Piet MT Broersen

Total Page:16

File Type:pdf, Size:1020Kb

Piet MT Broersen Automatic Autocorrelation and Spectral Analysis Piet M.T. Broersen Automatic Autocorrelation and Spectral Analysis With 104 Figures 123 Piet M.T. Broersen, PhD Department of Multi Scale Physics Delft University of Technology Kramers Laboratory Prins Bernhardlaan 6 2628 BW, Delft The Netherlands British Library Cataloguing in Publication Data Broersen, Piet M. T. Automatic autocorrelation and spectral analysis 1.Spectrum analysis - Statistical methods 2.Signal processing - Statistical methods 3.Autocorrelation (Statistics) 4.Time-series analysis I.Title 543.5’0727 ISBN-13: 9781846283284 ISBN-10: 1846283280 Library of Congress Control Number: 2006922620 ISBN-10: 1-84628-328-0 e-ISBN 1-84628-329-9 Printed on acid-free paper ISBN-13: 978-1-84628-328-4 © Springer-Verlag London Limited 2006 MATLAB®is a registered trademark of The MathWorks, Inc., 3 Apple Hill Drive, Natick, MA 01760-2098, U.S.A. http://www.mathworks.com Apart from any fair dealing for the purposes of research or private study, or criticism or review, as permitted under the Copyright, Designs and Patents Act 1988, this publication may only be reproduced, stored or transmitted, in any form or by any means, with the prior permission in writing of the publishers, or in the case of reprographic reproduction in accordance with the terms of licences issued by the Copyright Licensing Agency. Enquiries concerning reproduction outside those terms should be sent to the publishers. The use of registered names, trademarks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant laws and regulations and therefore free for general use. The publisher makes no representation, express or implied, with regard to the accuracy of the infor- mation contained in this book and cannot accept any legal responsibility or liability for any errors or omissions that may be made. Printed in Germany 987654321 Springer Science+Business Media springer.com To Rina Preface If different people estimate spectra from the same finite number of stationary stochastic observations, their results will generally not be the same. The reason is that several subjective decisions or choices have to be made during the current practice of spectral analysis, which influence the final spectral estimate. This applies also to the analysis of unique historical data about the atmosphere and the climate. That might be one of the reasons that the debate about possible climate changes becomes confused. The contribution of statistical signal processing can be that the same stationary statistical data will give the same spectral estimates for everybody who analyses those data. That unique solution will be acceptable only if it is close to the best attainable accuracy for most types of stationary data. The purpose of this book is to describe an automatic spectral analysis method that fulfills that requirement. It goes without saying that the best spectral description and the best autocorrelation description are strongly related because the Fourier transform connects them. Three different target groups can be distinguished for this book. Students in signal processing who learn how the power spectral density and the autocorrelation function of stochastic data can be estimated and interpreted with time series models. Several applications are shown. The level of mathe- matics is appropriate for students who want to apply methods of spectral analysis and not to develop them. They may be confident that more thorough mathematical derivations can be found in the referenced literature. Researchers in applied fields and all practical time series analysts who can learn that the combination of increased computer power, robust algorithms, and the improved quality of order selection have created a new and automatic time series solution for autocorrelation and spectral estimation. The increased computer power gives the possibility of computing enough candidate models such that there will always be a suitable candidate for given data. The improved order-selection quality always guarantees that one of the best candidates will be selected automatically and often the very best. The data themselves decide which is their best representation, and if desired, they suggest possible alter- natives. The automatic computer program ARMAsel provides their language. viii Preface Time series scientists who will observe that the methods and algorithms that are used to find a good spectral estimate are not always the methods that are preferred in asymptotic theory. The maximum likelihood theory especially has very good asymptotic theoretical properties, but the theory fails to indicate what sample sizes are required to benefit from those properties in practice. Maximum likelihood estimation often fails for moving average parameters. Furthermore, the most popular order-selection criterion of Akaike and the consistent criteria perform rather poorly in extensive Monte Carlo simulations. Asymptotic theory is concerned primarily with the optimal estimation of a single time series model with the true type and the true order, which are considered known. It should be a challenge to develop a sound mathematical background for finite-sample estimation and order selection. In finite-sample practice, models of different types and orders have to be computed because the truth is not yet known. This will always include models of too low orders, of too high orders, and of the wrong type. A good selection criterion has to pick the best model from all candidates. Good practical performance of simplified algorithms as a robust replacement for truly nonlinear estimation problems is not yet always understood. The time series theory in this book is limited to that part of the theory that I consider relevant for the user of an automatic spectral analysis method. Those subjects are treated that have been especially important in developing the program required to perform estimation automatically. The theory of time series models presents estimated models as a description of the autocorrelation function and the power spectral density of stationary stochastic data. A selection is made from the numerous estimation algorithms for time series models. A motivation of the choice of the preferred algorithms is given, often supported by simulations. For the description of many other methods and algorithms, references to the literature are given. The theory of windowed and tapered periodograms for spectra and lagged products for autocorrelation is considered critically. It is shown that those methods are not particularly suitable for stochastic processes and certainly not for automatic estimation. Their merit is primarily historical. They have been the only general, feasible, and practical solutions for spectral analysis for a long period until about 2002. In the last century, computers were not fast enough to compute many time series models, to select only one of them, and to forget the rest of the models. ARMAsel has become a useful time series solution for autocorrelation and spectral estimation by increased computer power, together with robust algorithms and improved order selection. Piet M.T. Broersen November 2005 Contents 1 Introduction ...................................................................................................... 1 1.1 Time Series Problems................................................................................ 1 2 Basic Concepts ................................................................................................ 11 2.1 Random Variables ................................................................................... 11 2.2 Normal Distribution ................................................................................ 14 2.3 Conditional Densities .............................................................................. 17 2.4 Functions of Random Variables .............................................................. 18 2.5 Linear Regression.................................................................................... 20 2.6 General Estimation Theory...................................................................... 23 2.7 Exercises.................................................................................................. 26 3 Periodogram and Lagged Product Autocorrelation.................................... 29 3.1 Stochastic Processes................................................................................ 29 3.2 Autocorrelation Function......................................................................... 31 3.3 Spectral Density Function ....................................................................... 33 3.4 Estimation of Mean and Variance ........................................................... 38 3.5 Autocorrelation Estimation ..................................................................... 40 3.6 Periodogram Estimation .......................................................................... 49 3.7 Summary of Nonparametric Methods ..................................................... 55 3.8 Exercises.................................................................................................. 56 4 ARMA Theory ................................................................................................ 59 4.1 Time Series Models................................................................................. 59 4.2 White Noise............................................................................................
Recommended publications
  • Power Comparisons of Five Most Commonly Used Autocorrelation Tests
    Pak.j.stat.oper.res. Vol.16 No. 1 2020 pp119-130 DOI: http://dx.doi.org/10.18187/pjsor.v16i1.2691 Pakistan Journal of Statistics and Operation Research Power Comparisons of Five Most Commonly Used Autocorrelation Tests Stanislaus S. Uyanto School of Economics and Business, Atma Jaya Catholic University of Indonesia, [email protected] Abstract In regression analysis, autocorrelation of the error terms violates the ordinary least squares assumption that the error terms are uncorrelated. The consequence is that the estimates of coefficients and their standard errors will be wrong if the autocorrelation is ignored. There are many tests for autocorrelation, we want to know which test is more powerful. We use Monte Carlo methods to compare the power of five most commonly used tests for autocorrelation, namely Durbin-Watson, Breusch-Godfrey, Box–Pierce, Ljung Box, and Runs tests in two different linear regression models. The results indicate the Durbin-Watson test performs better in the regression model without lagged dependent variable, although the advantage over the other tests reduce with increasing autocorrelation and sample sizes. For the model with lagged dependent variable, the Breusch-Godfrey test is generally superior to the other tests. Key Words: Correlated error terms; Ordinary least squares assumption; Residuals; Regression diagnostic; Lagged dependent variable. Mathematical Subject Classification: 62J05; 62J20. 1. Introduction An important assumption of the classical linear regression model states that there is no autocorrelation in the error terms. Autocorrelation of the error terms violates the ordinary least squares assumption that the error terms are uncorrelated, meaning that the Gauss Markov theorem (Plackett, 1949, 1950; Greene, 2018) does not apply, and that ordinary least squares estimators are no longer the best linear unbiased estimators.
    [Show full text]
  • LECTURES 2 - 3 : Stochastic Processes, Autocorrelation Function
    LECTURES 2 - 3 : Stochastic Processes, Autocorrelation function. Stationarity. Important points of Lecture 1: A time series fXtg is a series of observations taken sequentially over time: xt is an observation recorded at a specific time t. Characteristics of times series data: observations are dependent, become available at equally spaced time points and are time-ordered. This is a discrete time series. The purposes of time series analysis are to model and to predict or forecast future values of a series based on the history of that series. 2.2 Some descriptive techniques. (Based on [BD] x1.3 and x1.4) ......................................................................................... Take a step backwards: how do we describe a r.v. or a random vector? ² for a r.v. X: 2 d.f. FX (x) := P (X · x), mean ¹ = EX and variance σ = V ar(X). ² for a r.vector (X1;X2): joint d.f. FX1;X2 (x1; x2) := P (X1 · x1;X2 · x2), marginal d.f.FX1 (x1) := P (X1 · x1) ´ FX1;X2 (x1; 1) 2 2 mean vector (¹1; ¹2) = (EX1; EX2), variances σ1 = V ar(X1); σ2 = V ar(X2), and covariance Cov(X1;X2) = E(X1 ¡ ¹1)(X2 ¡ ¹2) ´ E(X1X2) ¡ ¹1¹2. Often we use correlation = normalized covariance: Cor(X1;X2) = Cov(X1;X2)=fσ1σ2g ......................................................................................... To describe a process X1;X2;::: we define (i) Def. Distribution function: (fi-di) d.f. Ft1:::tn (x1; : : : ; xn) = P (Xt1 · x1;:::;Xtn · xn); i.e. this is the joint d.f. for the vector (Xt1 ;:::;Xtn ). (ii) First- and Second-order moments. ² Mean: ¹X (t) = EXt 2 2 2 2 ² Variance: σX (t) = E(Xt ¡ ¹X (t)) ´ EXt ¡ ¹X (t) 1 ² Autocovariance function: γX (t; s) = Cov(Xt;Xs) = E[(Xt ¡ ¹X (t))(Xs ¡ ¹X (s))] ´ E(XtXs) ¡ ¹X (t)¹X (s) (Note: this is an infinite matrix).
    [Show full text]
  • Alternative Tests for Time Series Dependence Based on Autocorrelation Coefficients
    Alternative Tests for Time Series Dependence Based on Autocorrelation Coefficients Richard M. Levich and Rosario C. Rizzo * Current Draft: December 1998 Abstract: When autocorrelation is small, existing statistical techniques may not be powerful enough to reject the hypothesis that a series is free of autocorrelation. We propose two new and simple statistical tests (RHO and PHI) based on the unweighted sum of autocorrelation and partial autocorrelation coefficients. We analyze a set of simulated data to show the higher power of RHO and PHI in comparison to conventional tests for autocorrelation, especially in the presence of small but persistent autocorrelation. We show an application of our tests to data on currency futures to demonstrate their practical use. Finally, we indicate how our methodology could be used for a new class of time series models (the Generalized Autoregressive, or GAR models) that take into account the presence of small but persistent autocorrelation. _______________________________________________________________ An earlier version of this paper was presented at the Symposium on Global Integration and Competition, sponsored by the Center for Japan-U.S. Business and Economic Studies, Stern School of Business, New York University, March 27-28, 1997. We thank Paul Samuelson and the other participants at that conference for useful comments. * Stern School of Business, New York University and Research Department, Bank of Italy, respectively. 1 1. Introduction Economic time series are often characterized by positive
    [Show full text]
  • 3 Autocorrelation
    3 Autocorrelation Autocorrelation refers to the correlation of a time series with its own past and future values. Autocorrelation is also sometimes called “lagged correlation” or “serial correlation”, which refers to the correlation between members of a series of numbers arranged in time. Positive autocorrelation might be considered a specific form of “persistence”, a tendency for a system to remain in the same state from one observation to the next. For example, the likelihood of tomorrow being rainy is greater if today is rainy than if today is dry. Geophysical time series are frequently autocorrelated because of inertia or carryover processes in the physical system. For example, the slowly evolving and moving low pressure systems in the atmosphere might impart persistence to daily rainfall. Or the slow drainage of groundwater reserves might impart correlation to successive annual flows of a river. Or stored photosynthates might impart correlation to successive annual values of tree-ring indices. Autocorrelation complicates the application of statistical tests by reducing the effective sample size. Autocorrelation can also complicate the identification of significant covariance or correlation between time series (e.g., precipitation with a tree-ring series). Autocorrelation implies that a time series is predictable, probabilistically, as future values are correlated with current and past values. Three tools for assessing the autocorrelation of a time series are (1) the time series plot, (2) the lagged scatterplot, and (3) the autocorrelation function. 3.1 Time series plot Positively autocorrelated series are sometimes referred to as persistent because positive departures from the mean tend to be followed by positive depatures from the mean, and negative departures from the mean tend to be followed by negative departures (Figure 3.1).
    [Show full text]
  • Spatial Autocorrelation: Covariance and Semivariance Semivariance
    Spatial Autocorrelation: Covariance and Semivariancence Lily Housese ­P eters GEOG 593 November 10, 2009 Quantitative Terrain Descriptorsrs Covariance and Semivariogram areare numericc methods used to describe the character of the terrain (ex. Terrain roughness, irregularity) Terrain character has important implications for: 1. the type of sampling strategy chosen 2. estimating DTM accuracy (after sampling and reconstruction) Spatial Autocorrelationon The First Law of Geography ““ Everything is related to everything else, but near things are moo re related than distant things.” (Waldo Tobler) The value of a variable at one point in space is related to the value of that same variable in a nearby location Ex. Moranan ’s I, Gearyary ’s C, LISA Positive Spatial Autocorrelation (Neighbors are similar) Negative Spatial Autocorrelation (Neighbors are dissimilar) R(d) = correlation coefficient of all the points with horizontal interval (d) Covariance The degree of similarity between pairs of surface points The value of similarity is an indicator of the complexity of the terrain surface Smaller the similarity = more complex the terrain surface V = Variance calculated from all N points Cov (d) = Covariance of all points with horizontal interval d Z i = Height of point i M = average height of all points Z i+d = elevation of the point with an interval of d from i Semivariancee Expresses the degree of relationship between points on a surface Equal to half the variance of the differences between all possible points spaced a constant distance apart
    [Show full text]
  • Modeling and Generating Multivariate Time Series with Arbitrary Marginals Using a Vector Autoregressive Technique
    Modeling and Generating Multivariate Time Series with Arbitrary Marginals Using a Vector Autoregressive Technique Bahar Deler Barry L. Nelson Dept. of IE & MS, Northwestern University September 2000 Abstract We present a model for representing stationary multivariate time series with arbitrary mar- ginal distributions and autocorrelation structures and describe how to generate data quickly and accurately to drive computer simulations. The central idea is to transform a Gaussian vector autoregressive process into the desired multivariate time-series input process that we presume as having a VARTA (Vector-Autoregressive-To-Anything) distribution. We manipulate the correlation structure of the Gaussian vector autoregressive process so that we achieve the desired correlation structure for the simulation input process. For the purpose of computational efficiency, we provide a numerical method, which incorporates a numerical-search procedure and a numerical-integration technique, for solving this correlation-matching problem. Keywords: Computer simulation, vector autoregressive process, vector time series, multivariate input mod- eling, numerical integration. 1 1 Introduction Representing the uncertainty or randomness in a simulated system by an input model is one of the challenging problems in the practical application of computer simulation. There are an abundance of examples, from manufacturing to service applications, where input modeling is critical; e.g., modeling the time to failure for a machining process, the demand per unit time for inventory of a product, or the times between arrivals of calls to a call center. Further, building a large- scale discrete-event stochastic simulation model may require the development of a large number of, possibly multivariate, input models. Development of these models is facilitated by accurate and automated (or nearly automated) input modeling support.
    [Show full text]
  • Random Processes
    Chapter 6 Random Processes Random Process • A random process is a time-varying function that assigns the outcome of a random experiment to each time instant: X(t). • For a fixed (sample path): a random process is a time varying function, e.g., a signal. – For fixed t: a random process is a random variable. • If one scans all possible outcomes of the underlying random experiment, we shall get an ensemble of signals. • Random Process can be continuous or discrete • Real random process also called stochastic process – Example: Noise source (Noise can often be modeled as a Gaussian random process. An Ensemble of Signals Remember: RV maps Events à Constants RP maps Events à f(t) RP: Discrete and Continuous The set of all possible sample functions {v(t, E i)} is called the ensemble and defines the random process v(t) that describes the noise source. Sample functions of a binary random process. RP Characterization • Random variables x 1 , x 2 , . , x n represent amplitudes of sample functions at t 5 t 1 , t 2 , . , t n . – A random process can, therefore, be viewed as a collection of an infinite number of random variables: RP Characterization – First Order • CDF • PDF • Mean • Mean-Square Statistics of a Random Process RP Characterization – Second Order • The first order does not provide sufficient information as to how rapidly the RP is changing as a function of timeà We use second order estimation RP Characterization – Second Order • The first order does not provide sufficient information as to how rapidly the RP is changing as a function
    [Show full text]
  • On the Use of the Autocorrelation and Covariance Methods for Feedforward Control of Transverse Angle and Position Jitter in Linear Particle Beam Accelerators*
    '^C 7 ON THE USE OF THE AUTOCORRELATION AND COVARIANCE METHODS FOR FEEDFORWARD CONTROL OF TRANSVERSE ANGLE AND POSITION JITTER IN LINEAR PARTICLE BEAM ACCELERATORS* Dean S. Ban- Advanced Photon Source, Argonne National Laboratory, 9700 S. Cass Ave., Argonne, IL 60439 ABSTRACT It is desired to design a predictive feedforward transverse jitter control system to control both angle and position jitter m pulsed linear accelerators. Such a system will increase the accuracy and bandwidth of correction over that of currently available feedback correction systems. Intrapulse correction is performed. An offline process actually "learns" the properties of the jitter, and uses these properties to apply correction to the beam. The correction weights calculated offline are downloaded to a real-time analog correction system between macropulses. Jitter data were taken at the Los Alamos National Laboratory (LANL) Ground Test Accelerator (GTA) telescope experiment at Argonne National Laboratory (ANL). The experiment consisted of the LANL telescope connected to the ANL ZGS proton source and linac. A simulation of the correction system using this data was shown to decrease the average rms jitter by a factor of two over that of a comparable standard feedback correction system. The system also improved the correction bandwidth. INTRODUCTION Figure 1 shows the standard setup for a feedforward transverse jitter control system. Note that one pickup #1 and two kickers are needed to correct beam position jitter, while two pickup #l's and one kicker are needed to correct beam trajectory-angle jitter. pickup #1 kicker pickup #2 Beam Fast loop Slow loop Processor Figure 1. Feedforward Transverse Jitter Control System It is assumed that the beam is fast enough to beat the correction signal (through the fast loop) to the kicker.
    [Show full text]
  • Lecture 10: Lagged Autocovariance and Correlation
    Lecture 10: Lagged autocovariance and correlation c Christopher S. Bretherton Winter 2014 Reference: Hartmann Atm S 552 notes, Chapter 6.1-2. 10.1 Lagged autocovariance and autocorrelation The lag-p autocovariance is defined N X ap = ujuj+p=N; (10.1.1) j=1 which measures how strongly a time series is related with itself p samples later or earlier. The zero-lag autocovariance a0 is equal to the power. Also note that ap = a−p because both correspond to a lag of p time samples. The lag-p autocorrelation is obtained by dividing the lag-p autocovariance by the variance: rp = ap=a0 (10.1.2) Many kinds of time series decorrelate in time so that rp ! 0 as p increases. On the other hand, for a purely periodic signal of period T , rp = cos(2πp∆t=T ) will oscillate between 1 at lags that are multiples of the period and -1 at lags that are odd half-multiples of the period. Thus, if the autocorrelation drops substantially below zero at some lag P , that usually corresponds to a preferred peak in the spectral power at periods around 2P . More generally, the autocovariance sequence (a0; a1; a2;:::) is intimately re- lated to the power spectrum. Let S be the power spectrum deduced from the DFT, with components 2 2 Sm = ju^mj =N ; m = 1; 2;:::;N (10.1.3) Then one can show using a variant of Parseval's theorem that the IDFT of the power spectrum gives the lagged autocovariance sequence. Specif- ically, let the vector a be the lagged autocovariance sequence (acvs) fap−1; p = 1;:::;Ng computed in the usual DFT style by interpreting indices j + p outside the range 1; ::; N periodically: j + p mod(j + p − 1;N) + 1 (10.1.4) 1 Amath 482/582 Lecture 10 Bretherton - Winter 2014 2 Note that because of the periodicity an−1 = a−1, i.
    [Show full text]
  • Autocorrelation
    Autocorrelation David Gerbing School of Business Administration Portland State University January 30, 2016 Autocorrelation The difference between an actual data value and the forecasted data value from a model is the residual for that forecasted value. Residual: ei = Yi − Y^i One of the assumptions of the least squares estimation procedure for the coefficients of a regression model is that the residuals are purely random. One consequence of randomness is that the residuals would not correlate with anything else, including with each other at different time points. A value above the mean, that is, a value with a positive residual, would contain no information as to whether the next value in time would have a positive residual, or negative residual, with a data value below the mean. For example, flipping a fair coin yields random flips, with half of the flips resulting in a Head and the other half a Tail. If a Head is scored as a 1 and a Tail as a 0, and the probability of both Heads and Tails is 0.5, then calculate the value of the population mean as: Population Mean: µ = (0:5)(1) + (0:5)(0) = :5 The forecast of the outcome of the next flip of a fair coin is the mean of the process, 0.5, which is stable over time. What are the corresponding residuals? A residual value is the difference of the corresponding data value minus the mean. With this scoring system, a Head generates a positive residual from the mean, µ, Head: ei = 1 − µ = 1 − 0:5 = 0:5 A Tail generates a negative residual from the mean, Tail: ei = 0 − µ = 0 − 0:5 = −0:5 The error terms of the coin flips are independent of each other, so if the current flip is a Head, or if the last 5 flips are Heads, the forecast for the next flip is still µ = :5.
    [Show full text]
  • Central Limit Theorems When Data Are Dependent: Addressing the Pedagogical Gaps
    Institute for Empirical Research in Economics University of Zurich Working Paper Series ISSN 1424-0459 Working Paper No. 480 Central Limit Theorems When Data Are Dependent: Addressing the Pedagogical Gaps Timothy Falcon Crack and Olivier Ledoit February 2010 Central Limit Theorems When Data Are Dependent: Addressing the Pedagogical Gaps Timothy Falcon Crack1 University of Otago Olivier Ledoit2 University of Zurich Version: August 18, 2009 1Corresponding author, Professor of Finance, University of Otago, Department of Finance and Quantitative Analysis, PO Box 56, Dunedin, New Zealand, [email protected] 2Research Associate, Institute for Empirical Research in Economics, University of Zurich, [email protected] Central Limit Theorems When Data Are Dependent: Addressing the Pedagogical Gaps ABSTRACT Although dependence in financial data is pervasive, standard doctoral-level econometrics texts do not make clear that the common central limit theorems (CLTs) contained therein fail when applied to dependent data. More advanced books that are clear in their CLT assumptions do not contain any worked examples of CLTs that apply to dependent data. We address these pedagogical gaps by discussing dependence in financial data and dependence assumptions in CLTs and by giving a worked example of the application of a CLT for dependent data to the case of the derivation of the asymptotic distribution of the sample variance of a Gaussian AR(1). We also provide code and the results for a Monte-Carlo simulation used to check the results of the derivation. INTRODUCTION Financial data exhibit dependence. This dependence invalidates the assumptions of common central limit theorems (CLTs). Although dependence in financial data has been a high- profile research area for over 70 years, standard doctoral-level econometrics texts are not always clear about the dependence assumptions needed for common CLTs.
    [Show full text]
  • Wavelets, Their Autocorrelation Functions, and Multiresolution Representation of Signals
    Wavelets, their autocorrelation functions, and multiresolution representation of signals Gregory Beylkin University of Colorado at Boulder, Program in Applied Mathematics Boulder, CO 80309-0526 Naoki Saito 1 Schlumberger–Doll Research Old Quarry Road, Ridgefield, CT 06877-4108 ABSTRACT We summarize the properties of the auto-correlation functions of compactly supported wavelets, their connection to iterative interpolation schemes, and the use of these functions for multiresolution analysis of signals. We briefly describe properties of representations using dilations and translations of these auto- correlation functions (the auto-correlation shell) which permit multiresolution analysis of signals. 1. WAVELETS AND THEIR AUTOCORRELATION FUNCTIONS The auto-correlation functions of compactly supported scaling functions were first studied in the context of the Lagrange iterative interpolation scheme in [6], [5]. Let Φ(x) be the auto-correlation function, +∞ Φ(x)= ϕ(y)ϕ(y x)dy, (1.1) Z−∞ − where ϕ(x) is the scaling function which appears in the construction of compactly supported wavelets in [3]. The function Φ(x) is exactly the “fundamental function” of the symmetric iterative interpolation scheme introduced in [6], [5]. Thus, there is a simple one-to-one correspondence between iterative interpolation schemes and compactly supported wavelets [12], [11]. In particular, the scaling function corresponding to Daubechies’s wavelet with two vanishing moments yields the scheme in [6]. In general, the scaling functions corresponding to Daubechies’s wavelets with M vanishing moments lead to the iterative interpolation schemes which use the Lagrange polynomials of degree 2M [5]. Additional variants of iterative interpolation schemes may be obtained using compactly supported wavelets described in [4].
    [Show full text]