Abstract
As we have previously stated on a number of occasions, if g is integrable, its Hilbert transform is not necessarily integrable. Moreover, it can be even not locally integrable. When the Hilbert transform is integrable, we say that g is in the (real) Hardy space H1: = H1(ℝ). There are a variety of its characterizations (or, equivalently, definitions). The one given by means of the Hilbert transform is both important and convenient.
Original language | English |
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Title of host publication | Pathways in Mathematics |
Publisher | Birkhauser |
Pages | 101-129 |
Number of pages | 29 |
DOIs | |
State | Published - 2021 |
Publication series
Name | Pathways in Mathematics |
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ISSN (Print) | 2367-3451 |
ISSN (Electronic) | 2367-346X |
Bibliographical note
Publisher Copyright:© 2021, The Author(s), under exclusive license to Springer Nature Switzerland AG.