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2020 | OriginalPaper | Chapter

3. Distribution Theory by Riemann Integrals

Authors : Hans G. Feichtinger, Mads S. Jakobsen

Published in: Mathematical Modelling, Optimization, Analytic and Numerical Solutions

Publisher: Springer Singapore

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Abstract

It is the purpose of this article to outline a syllabus for a course that can be given to engineers looking for an understandable mathematical description of the foundations of distribution theory and the necessary functional analytic methods. Arguably, these are needed for a deeper understanding of basic questions in signal analysis. Objects such as the Dirac delta and the Dirac comb should have a proper definition, and it should be possible to explain how one can reconstruct a band-limited function from its samples by means of simple series expansions. It should also be useful for graduate mathematics students who want to see how functional analysis can help to understand fairly practical problems, or teachers who want to offer a course related to the “Mathematical Foundations of Signal Processing” at their institutions. The course requires only an understanding of the basic terms from linear functional analysis, namely Banach spaces and their duals, bounded linear operators, and a simple version of \( w^{*} \)-convergence. As a matter of fact, we use a set of function spaces which is quite different from the collection of Lebesgue spaces \((L^p(\mathbb {R}_d),\Vert .\Vert _p)\) used normally. We thus avoid the use of the Lebesgue integration theory. Furthermore, we avoid topological vector spaces in the form of the Schwartz space. Although practically all the tools developed and presented can be realized in the context of LCA (locally compact abelian) groups, i.e., in the most general setting where a (commutative) Fourier transform makes sense, we restrict our attention in the current presentation to the Euclidean setting, where we have (generalized) functions over \(\mathbb {R}^d\). This allows us to make use of simple BUPUs (bounded, uniform partitions of unity), to apply dilation operators and occasionally to make use of concrete special functions such as the (Fourier invariant) standard Gaussian, given by \(g_0(t) = \exp (- \pi \vert t \vert ^{2})\). The problems of the overall current situation, with the separation of theoretical Fourier analysis as carried out by (pure) mathematicians and Applied Fourier analysis (as used in engineering applications) are getting bigger and bigger and therefore courses filling the gap are in strong need. This note provides an outline and may serve as a guideline. The first author has given similar courses over the past years at different schools (ETH Zürich, DTU Lyngby, TU Munich, and currently Charles University Prague) and so one can claim that the outline is not just another theoretical contribution to the field.

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Footnotes
1
Commonly the term “infinite dimensional” is used, and we will also use it later on, but this expression wrongly suggests that instead of a finite basis one just has an infinite basis and this is not what we should expect or use!
 
2
Even if \((B,\Vert \cdot \Vert _B)\) is just a normed space.
 
3
Technically speaking, for separable Banach spaces \((B,\Vert \cdot \Vert _B)\) which are those that contain a countable, dense subset. This will be the case for all the situations where we make use of this concept.
 
4
\(B_R(0)\) is the ball of radius \(R > 0\) around zero in \(\mathbb {R}^d\).
 
5
What we denote by \(\delta _{x}\) is often called the Dirac delta function and denoted by \(\delta _{x}(t)\) or \(\delta (t-x)\) (the argument indicating that it is a “function” of, e.g., a time variable t). We do not view the Dirac delta in this way.
 
6
See the lectures notes on “Harmonic and Functional Analysis” at https://​www.​univie.​ac.​at/​nuhag-php/​home/​skripten.​php.
 
7
Also called Feichtinger’s algebra in the literature.
 
8
It is also a well-defined function in \(C_b(\mathbb {R}^{2d})\), or for \(g,f \in L^2(\mathbb {R}^d)\) making use of Lebesgue integration, the usual way of introducing the STFT.
 
9
In the book [40], and since then, the space \(S_0\) has been called the Feichtinger algebra.
 
10
This is comparable with the multiplication of real numbers which is defined as the limit of products of decimal approximations of the involved real numbers, and taking limits afterward!
 
11
The word “cardinal” comes into the picture because of the Lagrange type interpolation property of the function \(\text{ sinc }\): \(\text{ sinc }(k)=\delta _{k,0}\).
 
12
Recall that digital audio recordings are meant to capture all the frequencies up to 20 kHz and work with 44100 samples per second although the abstract Nyquist criterion would only ask for \(2 * 20000 = 40000\) samples per second (to express the Nyquist criterion in a practical form). Clearly the use of this theorem in a real-time situation requires the reconstruction being well localized in time, in order to cause only minimal delay of the reconstruction process.
 
13
But still much more has to be done!
 
14
This is well justified by the Riesz representation theorem.
 
15
In the terminology of Banach modules, we are talking about the fact that both \(S_0(\mathbb {R}^d)\) and \(S_0'(\mathbb {R}^d)\) are Banach modules over the Banach convolution algebra \((L^1(\mathbb {R}^d),\Vert \cdot \Vert _1)\), and that we are interested in the Banach module homomorphisms.
 
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Metadata
Title
Distribution Theory by Riemann Integrals
Authors
Hans G. Feichtinger
Mads S. Jakobsen
Copyright Year
2020
Publisher
Springer Singapore
DOI
https://doi.org/10.1007/978-981-15-0928-5_3

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