Skip to main content
Top

2002 | Book

Summability of Multi-Dimensional Fourier Series and Hardy Spaces

Author: Ferenc Weisz

Publisher: Springer Netherlands

Book Series : Mathematics and Its Applications

insite
SEARCH

About this book

The history of martingale theory goes back to the early fifties when Doob [57] pointed out the connection between martingales and analytic functions. On the basis of Burkholder's scientific achievements the mar­ tingale theory can perfectly well be applied in complex analysis and in the theory of classical Hardy spaces. This connection is the main point of Durrett's book [60]. The martingale theory can also be well applied in stochastics and mathematical finance. The theories of the one-parameter martingale and the classical Hardy spaces are discussed exhaustively in the literature (see Garsia [83], Neveu [138], Dellacherie and Meyer [54, 55], Long [124], Weisz [216] and Duren [59], Stein [193, 194], Stein and Weiss [192], Lu [125], Uchiyama [205]). The theory of more-parameter martingales and martingale Hardy spaces is investigated in Imkeller [107] and Weisz [216]. This is the first mono­ graph which considers the theory of more-parameter classical Hardy spaces. The methods of proofs for one and several parameters are en­ tirely different; in most cases the theorems stated for several parameters are much more difficult to verify. The so-called atomic decomposition method that can be applied both in the one-and more-parameter cases, was considered for martingales by the author in [216].

Table of Contents

Frontmatter
Chapter 1. Multi-Dimensional Dyadic Hardy Spaces
Abstract
The theory of the one-dimensional classical Hardy spaces are described in the books Duren [59], Stein [193, 194], Stein and Weiss [192], Lu [125] and Uchiyama [205] in details (see also Fefferman and Stein [67]). Motivated by the works of Burkholder, Davis and Gundy [21, 20, 52], the one-dimensional martingale Hardy spaces are investigated in Garsia [83], Neveu [138], Dellacherie and Meyer [54, 55], Long [124] and Weisz [216]. With the help of the Brownian motion one can find a strong connection between these two types of Hardy spaces (see Durrett [60] and Bass [4]).
Ferenc Weisz
Chapter 2. Multi-Dimensional Classical Hardy Spaces
Abstract
In this chapter the classical Hardy spaces on ℝ d and T d are introduced and all the results of Chapter 1 are proved for the classical spaces. As in Chapter 1, the various characterizations of the Hardy spaces are not proved. For these characterizations see the very nice and good books and papers of Duren [59], Stein [193, 194], Stein and Weiss [192], Lu [125], Uchiyama [205], Fefferman and Stein [67], Chang and Fefferman [33, 31, 71, 73] as well as Gundy and Stein [98, 100].
Ferenc Weisz
Chapter 3. Summability of D-Dimensional Walsh-Fourier Series
Abstract
In this chapter we consider the Cesàro and Riesz summability of multiparameter Walsh-Fourier series. For summations of the trigonometric-Fourier series see Chapter 5.
Ferenc Weisz
Chapter 4. The D-Dimensional Dyadic Derivative
Abstract
We have proved in Corollary 2.5 that
if fL 1[0, 1). The dyadic analogue of this result can be formulated as follows.
Ferenc Weisz
Chapter 5. Summability of D-Dimensional Trigonometric-Fourier Series
Abstract
In this section we consider the θ-summability of multi-parameter tri­gonometric-Fourier series.
Ferenc Weisz
Chapter 6. Summability of D-Dimensional Fourier Transforms
Abstract
In this chapter all the results from Chapter 5 are verified for d-dimensional Fourier transforms and tempered distributions. Here the L p,q and Hardy-Lorentz spaces H p,q and H p,q defined on ℝ d are consid­ered.
Ferenc Weisz
Chapter 7. Spline and Ciesielski Systems
Abstract
In the first four sections we consider the Kronecker product of the unbounded Ciesielski or spline systems of order (m j , k j ) introduced by Ciesielski [38, 45, 46] and the Hardy spaces and defined by the L p,q norms of the non-tangential maximal functions. Note that if k j = m j + 1 for all j then we obtain the usual dyadic Hardy spaces, in other cases H p,q is the restriction of the classical H p,q space to the unit cube. It is known that and are biorthogonal systems and that is the Haar system if m j = −1, k j = 0, the Franklin system if m j =0, k j =0.
Ferenc Weisz
Backmatter
Metadata
Title
Summability of Multi-Dimensional Fourier Series and Hardy Spaces
Author
Ferenc Weisz
Copyright Year
2002
Publisher
Springer Netherlands
Electronic ISBN
978-94-017-3183-6
Print ISBN
978-90-481-5992-5
DOI
https://doi.org/10.1007/978-94-017-3183-6