EXTENSIONS OF HARDY SPACES AND THEIR USE IN ANALYSIS
EXTENSIONS OF HARDY SPACES AND THEIR USE IN ANALYSIS
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DOI:
10.1090/s0002-9904-1977-14325-5
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发表时间:
1977-01-01
影响因子:
1.3
通讯作者:
WEISS, G
中科院分区:
文献类型:
--
作者:
COIFMAN, RR;WEISS, G
1. Introduction. It is well known that the theory of functions plays an important role in the classical theory of Fourier series. Because of this certain function spaces, the Hp spaces, have been studied extensively in harmonic analysis. When p> 1, If and Hp are essentially the same; however, when p< 1 the space Hp {% much better adapted to problems arising in the theory of Fourier series. We shall examine some of the properties of Hp for p< 1 and describe ways in which these spaces have been characterized recently. These characterizations enable us to extend their definition to a very general setting that will allow us to unify the study of many extensions of classical harmonic analysis.The theory of Hp spaces on Rn has recently received an important impetus from the work of C. Fefferman and EM Stein [29]. Their work resulted in many applications involving sharp estimates for convolution operators. It is not immediately apparent how much of a role the differential structure of R" plays in obtaining these results. Our purpose is to isolate from this theory some of the measure theoretic and geometric properties that enable us to obtain in a unified form many of these applications as well as other results in harmonic analysis. We shall not deal with those questions involving Hp spaces that are not relevant to our purpose. Some general references involving harmonic analysis and Hp spaces are [23],[64],[27],[62],[57] and [55]. The main tool in our development is an extension and a refinement of the Calderón-Zygmund decomposition of a function into a" good" and" bad'* part. This tool is presented in the proof of Theorem A and is of a somewhat technical nature. It is included here in order to make the presentation of the theory we develop essentially self-contained. In some examples we give applications of this theory that require material not presented here. We do, however, give the necessary references. In this sense, we hope that this exposition is accessible to a general audience* Before beginning our presentation we would like to thank our colleagues A. Baernstein, Y. Meyer, R. Rochberg and EM Stein who read a large part of this manuscript and made many useful suggestions. Suppose ƒ is a real-valued integrable function on T, the perimeter of the unit disc in the plane (which we identify in the usual way with [-7T, TT)). Suppose ƒ