4.4 Article

Weak Musielak-Orlicz Hardy spaces and applications

Journal

MATHEMATISCHE NACHRICHTEN
Volume 289, Issue 5-6, Pages 634-677

Publisher

WILEY-V C H VERLAG GMBH
DOI: 10.1002/mana.201500152

Keywords

Musielak-Orlicz function; weak Musielak-Orlicz Hardy space; maximal function; atom; molecule; Littlewood-Paley operator; Calderon-Zygmund operator

Categories

Funding

  1. National Natural Science Foundation of China [11571039, 11361020, 11301029]
  2. Specialized Research Fund for the Doctoral Program of Higher Education of China [20120003110003]
  3. Fundamental Research Funds for Central Universities of China [2013YB60, 2014KJJCA10]

Ask authors/readers for more resources

Let. : R n x [0,8). [0,8) satisfy that.(x, u), for any given x. R n, is an Orlicz function and.(u, t) is a Muckenhoupt A8(R n) weight uniformly in t. (0,8). In this article, the authors introduce the weak Musielak-Orlicz Hardy space WH.(R n) via the grand maximal function and then obtain its vertical or its nontangential maximal function characterizations. The authors also establish other real-variable characterizations of WH.(R n), respectively, in terms of the atom, the molecule, the Lusin area function, the Littlewood-Paley g-function or g*. -function. All these characterizations for weighted weak Hardy spaces WHp w (R n) (namely,.(x, t) := w(x) t p for all t. [0,8) and x. R n with p. (0, 1] and w. A8(R n)) are new and part of these characterizations even for weak Hardy spaces WHp(R n) (namely,.(x, t) := t p for all t. [0,8) and x. R n with p. (0, 1]) are also new. As an application, the boundedness of Calder ' on-Zygmund operators from H.(R n) to WH.(R n) in the critical case is presented.

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