<p>Let <i>p</i>(·): ℝ<sup><i>n</i></sup> → (0, ∞] be a variable exponent function satisfying the globally log-Hölder continuous condition and <i>A</i> a general expansive matrix on ℝ<sup><i>n</i></sup>. Let H<Stack> <sub><i>A</i></sub> <sup><i>p</i>(·)</sup> </Stack>(ℝ<sup><i>n</i></sup>) be the variable anisotropic Hardy space associated with <i>A</i>. In this paper, via first establishing a criterion for affirming some functions being in the space <i>H</i><Stack> <sub><i>A</i></sub> <sup><i>p</i>(·)</sup> </Stack>(ℝ<sup><i>n</i></sup>), the authors obtain several equivalent characterizations of <i>H</i><Stack> <sub><i>A</i></sub> <sup><i>p</i>(·)</sup> </Stack>(ℝ<sup><i>n</i></sup>) in terms of the so-called tight frame multiwavelets, which extend the well-known wavelet characterizations of classical Hardy spaces. In particular, these wavelet characterizations are shown without the help of Peetre maximal operators.</p>

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Wavelet Characterizations of Variable Anisotropic Hardy Spaces

  • Yao He,
  • Yong Jiao,
  • Jun Liu

摘要

Let p(·): ℝn → (0, ∞] be a variable exponent function satisfying the globally log-Hölder continuous condition and A a general expansive matrix on ℝn. Let H A p(·) (ℝn) be the variable anisotropic Hardy space associated with A. In this paper, via first establishing a criterion for affirming some functions being in the space H A p(·) (ℝn), the authors obtain several equivalent characterizations of H A p(·) (ℝn) in terms of the so-called tight frame multiwavelets, which extend the well-known wavelet characterizations of classical Hardy spaces. In particular, these wavelet characterizations are shown without the help of Peetre maximal operators.