DISTRIBUTION THEORY AND TRANSFORM ANALYSIS
A.H. Zemanian

PREFACE

L. Schwartz's theory of distributions had two important effects in
mathematical analysis. First of all, it provided a rigorous justification
for a number of formal manipulations that had become quite common in
the technical literature. The second and more important effect was
that it opened up a new area of mathematical research, which in turn
provided an impetus in the development of a number of mathematical
disciplines, such as ordinary and partial differential equations, operational
calculus, integral-transformation theory, and functional analysis.
However, the subject has remained pretty much in the realm of advanced
mathematics, and only a few aspects of it have found their way into the
technical literature.

To be sure, a certain type of distribution (in particular, the delta
function and its derivatives) had been used in the physical and engineering
sciences for quite some time before the advent of distribution theory.
Indeed, the delta function dates back to the nineteenth century. A summary
of its history is given by Van der Pol and Bremmer. On the other hand,
distribution theory appears to have first been formulated in 1936 by S.L.Soboleff
and then developed in a systematic and thorough way by L. Schwartz, whose books appeared
in 1950 and 1951. A somewhat different version of this theory was proposed by S. Bochner
around 1927, who used it to generalize the Fourier transformation for
functions f(t) that grow as some power of t as |t| approaches infinity.

This book, which is based on a graduate course given at the State
University of New York at Stony Brook, has two objectives. The first
is to provide a comparatively elementary introduction to distribution
theory, and the second is to describe the generalized Fourier and Laplace
transformations and their applications to integrodifferential equations,
difference equations, and passive systems. In recent years an ever-increasing number
of textbooks have been devoted to the classical Fourier and Laplace
transformations. The corresponding distributional transformations,
although they are considerably more powerful tools, have not received
the same attention in the current textbooks, nor have they been widely employed
by scientists and engineers. It is hoped that this book will help to popularize
distributional transform analysis.

Actually, one can introduce the delta function and its derivatives
without developing a general theory of distributions, and many current
books do so. However, these singular functions comprise but a very
small class of all the distributions. More importantly, distribution
theory provides powerful analytical techniques that cannot be described
merely in terms of the delta function and its derivatives. An account
of some of these techniques is given in this book.

Another theory of generalized functions is provided by Mikusinski's
operational calculus, which is related to the distributional Laplace transformation
in roughly the same way as Heaviside's operational calculus is related
to the classical Laplace transformation. In many problems one can use either
Mikusinski's method or the distributional technique to obtain a solution.
It is the latter procedure that is discussed in this book, and one possible
justification for it is the following. At the present time the classical
Laplace transformation has pretty much superseded Heaviside's operational
calculus both in the technical literature and in our college courses. It seems, therefore,
more natural to extend the Laplace transformation rather than Heaviside's
method and thereby build on the training that the student already has.
Admittedly, this is purely a pragmatic reason. Assuming
if you will, that time is of no importance, the best answer to the question
``Which theory should be studied?'' is ``Both.'' In Sec. 6.4, we very
briefly discuss Mikusinski's operational calculus and compare it with
distribution theory.

There are a variety of other approaches to the theory of generalized
functions that are based, in general, on the facts that generalized functions
can be represented as sequences of ordinary functions, which converge
in a certain way, and that over a finite interval a generalized function
is a finite-order derivative (in an unconventional sense) of a continuous function.
These methods can be understood in terms of Schwartz's theory,
and are, in fact, encompassed by it. If one wishes to delve at some length into the theory
of generalized functions, a knowledge of Schwartz's approach, which conceives of
generalized functions as certain continuous linear functionals, has become
indispensable, in view of the large and ever-increasing body of literature
that uses this point of view. For these reasons, our development will employ
Schwartz's functional approach.

This book can be used for a graduate course for engineering and science
students and possibly for a senior-level undergraduate course for
mathematics majors. It is presumed that the reader has already had a
course in advanced calculus and is familiar with the standard theorems
on the interchange of limit processes. Some knowledge of functions
of a complex variable and of matrix manipulations is also assumed.
Finally, at certain places we employ some elements of the theory of Lebesgue
integration, although most of the text can be followed without having
any knowledge of that subject. In any case, whenever theorems or techniques
in any of these subjects are used, the reader is referred to various
standard books, where he may seek any additional information that he may need.

An attempt has been made to render all the proofs as elementary as
possible. For example, Theorem 3.4-2 can be proved in a very brief
way if use is made of the Hahn-Banach theorem. This has not been done;
instead, a longer but more elementary argument has been employed.

Since this book is addressed to both mathematics students and to science
and engineering students, the problems have been designed to develop
the reader's understanding of the theory as well as his facility for using
distributions. Thus, some of the problems are exercises of proof; they are
concerned either with the arguments given in the text or with the extension
of the theory and the development of new results. In contrast to this,
other problems develop specific convolution and transform
formulas. Still others are exercises for solving distributionally
various differential and difference equations; they are intended to enlarge
the student's ability to apply distribution theory. It is hoped that a
sufficiently broad spectrum of problems has been provided to satisfy the
diverse needs of various types of students.

Briefly, the structure of this book is as follows. In Chapter 1 the
basic definitions of distributions and the operations that apply to them
are discussed. The calculus of distributions and, in particular, limits,
differentiation, integration, and the exchange of limiting processes are
considered in Chapter 2. Some deeper properties of distributions, such
as their local character as derivatives of continuous functions, are given
in Chapter 3.

Chapter 4 introduces distributions of slow growth, which arise naturally
in the generalization of the Fourier transformation. Chapters 5 and 6
are concerned with the convolution process and its use in representing
differential and difference equations.

The distributional Fourier and Laplace transformation are developed
in Chapters 7 and 8, and the latter transformation is applied in Chapter 9
to obtain an operational calculus for the solution of differential
and difference equations of the initial-condition type.

Some of the previous theory is applied in Chapter 10 to a discussion
of the fundamental properties of certain physical systems, and a concise
development of the relationship between the positive-reality of a system
function and the passivity of the system is obtained there.

Chapter 11 ends the book with a consideration of periodic distributions
This chapter acts in a crude way as a summary of the book, since it follows
the broad outline of the preceding portion of the text.

The appendices contain a table of formulas for the distributional
Laplace transformation, a glossary of symbols, and a bibliography. We
particularly direct the reader's attention to Appendix C, which contains
the definitions of most of the symbols used in the text.

There is enough material in this book for a two-semester course.
A one-semester course may be based upon th following portions of the text:
Secs. 1.1 to 1.8, 2.1 to 2.4, 2.6, 2.7, 3.1, 3.3, 3.4, 4.1 to 4.5, 5.1 to 5.6,
6.1 to 6.3, 7.1 to 7.5, 8.1 to 8.5, 9.1 to 9.6. These sections are self-contained;
indeed, for those wishing a more rapid introduction to the subject
without the more specialized or advanced discussions of the other sections,
this outline is a good one to follow. We have designated these sections
by using stars and diamonds. Sections denoted by diamonds are those
whose conclusions are used in the subsequent development of starred
and diamond-marked sections but whose proofs are fairly long and technical.
The reader may at first skip these proofs and just read the theorems,
examples, and explanatory portions of the diamond-marked sections.
This will provide a still briefer introduction to distribution theory
without any loss of continuity.

A.H. Zemanian
Stony Brook, New York