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Elements of Abstract Harmonic Analysis PDF

262 Pages·1964·4.332 MB·English
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ACADEMIC PAPERBACKS* BIOLOGY Edited by ALVIN NASON Design and Function at the Threshold of Life The Viruses HEINZ FRAENKEL-CONRAT Time, Cells, and Aging BERNARD L. STREHLER Isotopes in Biology GEORGE WOLF Life : Its Nature, Origin, and Development A I. OPARIN MATHEMATICS Edited by W. MAGNUS and A. SHENITZER Finite Permutation Groups HELMUT WIELANDT Introduction to p-Adic Numbers and Valuation Theory GEORGE BACHMAN Quadratic Forms and Matrices N. V. YEFIMOV Elements of Abstract Harmonic Analysis GEORGE BACHMAN Noneuclidean Geometry HERBERT MESCHKOWSKI PHYSICS Edited by D. ALLAN BROMLEY Elementary Dynamics of Particles H. W. HARKNESS Elementary Plane Rigid Dynamics H. W. HARKNESS Crystals: Their Role in Nature and in Science CHARLES BUNN Potential Barriers in Semiconductors B. R. GOSSICK Mössbauer Effect : Principles and Applications GÜNTHER K. WERTHEIM * Most of these volumes are also available in a cloth bound edition. Elements of Abstract Harmonic Analysis By George Bachman POLYTECHNIC INSTITUTE OF BROOKLYN DEPARTMENT OF MATHEMATICS BROOKLYN, NEW YORK with the assistance of Lawrence Narici POLYTECHNIC INSTITUTE OF BROOKLYN DEPARTMENT OF MATHEMATICS BROOKLYN, NEW YORK ACADEMIC PRESS A SUBSIDIARY OF HARCOURT BRACE JOVANOVICH, PUBLISHERS New York London Toronto Sydney San Francisco COPYRIGHT © 1964, BY ACADEMIC PRESS INC. ALL RIGHTS RESERVED. NO PART OF THIS BOOK MAY BE REPRODUCED IN ANY FORM, BY PHOTOSTAT, MICROFILM, OR ANY OTHER MEANS, WITHOUT WRITTEN PERMISSION FROM THE PUBLISHERS. ACADEMIC PRESS INC. Ill Fifth Avenue, New York, New York 10003 United Kingdom Edition published by ACADEMIC PRESS, INC. (LONDON) LTD. 24/28 Oval Road, London NW1 LIBRARY OF CONGRESS CATALOG CARD NUMBER: 64-21663 PRINTED IN THE UNITED STATES OF AMERICA 81 82 9 8 7 6 5 4 32 Preface Abstract Harmonic Analysis is an active branch of modern analysis which is increasing in importance as a standard course for the beginning graduate student. Concepts like Banach algebras, Haar measure, locally compact Abelian groups, etc., appear in many current research papers. This book is intended to enable the student to approach the original literature more quickly by informing him of these concepts and the basic theorems involving them. In order to give a reasonably complete and self-contained introduction to the subject, most of the proofs have been presented in great detail thereby making the development understandable to a very wide audience. Exercises have been supplied at the end of each chapter. Some of these are meant to extend the theory slightly while others should serve to test the reader's understanding of the material presented. The first chapter and part of the second give a brief review of classical Fourier analysis and present concepts which will subsequently be generalized to a more abstract framework. The presentation of this material is not meant to be detailed but is given mainly to motivate the generaliza- tions obtained later in the book. The next five chapters pre- sent an introduction to commutative Banach algebras, gen- eral topological spaces, and topological groups. We hope that Chapters 2-6 might serve as an adequate introduction for those students primarily interested in the theory of com- mutative Banach algebras as well as serving as needed pre- requisite material for the abstract harmonic analysis. The remaining chapters contain some of the measure theoretic background, including the Haar integral, and an extension of the concepts of the first two chapters to Fourier analysis on locally compact topological abelian groups. In an attempt to make the book as self-contained and as introductory as possible, it was felt advisable to start from scratch with many concepts—in particular with general v VI Preface topological spaces. However, within the space limitations, it was not possible to do this with certain other background material—notably some measure theory and a few facts from functional analysis. Nevertheless, the material needed from these areas has all been listed in various appendices to the chapters to which they are most relevant. There are now a number of more advanced books on abstract harmonic analysis which go deeper into the subject. We cite in particular the references to Rudin, Loomis, and the recent book by Hewitt and Ross. Our treatment of the latter part of Chapter 12 follows to some extent the initial chapter of the book by Rudin, which would be an excellent continuation for the reader who wishes to pursue these matters further. The present book is based on a one semester course in abstract harmonic analysis given at the Polytechnic In- stitute of Brooklyn during the summer of 1963, for which lecture notes were written by Lawrence Narici. A few re- visions and expansions have been made. I would like to express my sincere gratitude to Mr. Narici for his effort in writing the notes, improving many of the proofs, and for editing the entire manuscript. I would like finally to express also my appreciation to Melvin Maron for his help in the preparation of the manuscript. GEORGE BACHMAN Symbols Used in Text {x I p] The set of all x with property p f : X —► Y The function / mapping the set X into the set Y x —» y where x £ X is mapped into y Ç F. Further, if E <Z X, f(E) will denote the image set of 2? under /; i.e., /(#) = {/(x) | x Ç #}. If # C YJ~l(M) will denote those x ζ X such that/(x) 6 M. The notation/ |,, E QX, will denote the restriction of / to E. CE The complement of the set E 0 The null set C The complex numbers In the list below the number immediately following the symbol will denote the page on which the symbol is defined. The symbols are listed according to the order in which they appear in the text. R, 1 Ô, 61 L„ 1 Ê, 62 11/IU 2; ||/||X) 180; £·, 71 11/IL 196 V(x), 66 f*g, 6,180 ν {M; Χι, Χ2, ···, χ„, «ί)),, 8877 /, 2 C*, 99 L(X, X), 26 Ä*, 99 la(Z), 28 F,F = xy\x {zy\x€V yÇVt}, || A ||, A eL(X,X), 26 2 h 100 CO, 6], 26 W, 26 f/-1 = {a;-1 \x€ U], 100 Z, 28 (?/#, 110 lim/(s), 116 σ(χ), 37 s ßx, 41 r.(x), 42 X*, 118 M, 52 C, 125 x(M), M £ M, 51 M, 126 F (M), 57 Co (G), 129 X Symbols Used in Text xi Co+«7), 129 /*(*), /(ar>), 188 ki, 129 Ä(G), 193 (/:*), 130 X, 193 IM), 136 /(x), 193 /(/), 157 N( E, ), 204 X(h e μ*, 161 !*((?), 220 £*, £». 177 Z?(X), B(Y), 212 /„ /„, 177, 188 μ * v, 214 Li((?), 180 N(xo,E ), 222 >e CHAPTER 1 The Fourier Transform on the Real Line for Functions in L { Introduction This section will be devoted to some Fourier analysis on the real line. The notion of convolution will be introduced and some relationships between functions and their trans- forms will be derived. Some ideas from real variables (e.g. passage to the limit under the Lebesgue integral and inter- changing the order of integration in iterated integrals) will be heavily relied upon and a summary of certain theorems that will be used extensively in this section are included in the appendix at the end of this chapter. Notation Throughout, R will denote the real axis, ( — <*>, oo ), and / will denote a measurable function on R ( / may be real or complex valued). We will denote by L the set of all meas- p urable functions on R with the property f \f(x) \pdx < oo, 1 < p < /: Also, since we will so frequently be integrating from minus infinity to plus infinity, we will denote / by simply / J—oo J where all integrations are taken in the Lebesgue sense. t One often says that / is pth power summable. 1 2 Elements of Abstract Harmonic Analysis Noting without proof that the space L is a linear space p we can now define the norm off with respect top, \\ f \\ , where p / £ L as follows: p \1/P ,, ll/ll* = (/l/(*)l <fc It is simple to verify that the following assertions are valid: 1. U/H, > 0 and ||/|| = 0 if and only if /~0.f p 2. || A/||p = I Ä ΙΊΙ/UP where A; is a real or complex number. Note that this immediately implies ||/ || = p Il-/IL, 3. \\f + g \\ < ||/||p + \\g \\ . To verify this all one P P needs is Minkowski's inequality for integrals which is listed in the appendix to this chapter (p. 15). Thus it is seen that L is a normed linear space. One can p go one step further however; although it will not be proven here, it turns out that L is actually a complete normed linear p space or Banach space, or that any Cauchy sequence (in the norm with respect to p) of functions in L converges (in the p norm with respect to p) to a function that is pth. power summable. The Fourier Transform In this section we consider the Fourier transform of a function / in L\ and note certain properties of the Fourier transform. Let / 6 Li and consider as the Fourier transform of/ f(x) = feixtf(t) dt. t We will say that two functions, / and g, are equivalent, denoted by / ~ g, if / = g almost everywhere. Thus L is actually the set of all p equivalence classes of functions under this equivalence relation. If we did not do this then || || would represent a pseudonorm because it p would be possible for 11 /11„ to equal zero even though / was not zero. 1. Fourier Transform for Functions in Li 3 We first note that f(x) exists for, since / Ç L h \f(x) I < f\f(t)\dt< ». Further, since f\f(t)\dt= ||/1|! we can say l/(*)l < ll/lli for any x; or that the 1-norm of / is an upper bound for the Fourier transform of /. Since it is an upper bound it is cer- tainly greater than or equal to the least upper bound or sup I /(*) | < U/H,. It will now be shown that the Fourier transform of / is a continuous function of x. Consider the difference f(x + K) - f(x) = fe**'(e*·' - l)f(t) dt where h ζ R: n I f(x + K) - f(x) I < / I exp(ih t) - 1 | |/(0 | dt. n Since this is true for any h it is true in the limit as h ap- n n proaches zero, or lim | f(x + h ) - f(x) | < lim /" | e*·' - 1 | |/(0 | dt. n Our wish now is to take the limit operation under the inte- gral sign, and LebesguVs dominated convergence theorem will allow this manipulation (see appendix to Chapter 1) for certainly the integrand in the last expression is dominated

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