Characterization of the atomic space $H^1$ for non doubling measures in terms of a grand maximal operator

dc.creatorTolsa, Xavier
dc.date2000-05-06
dc.date.accessioned2026-07-07T04:35:03Z
dc.date.available2026-07-07T04:35:03Z
dc.descriptionLet $μ$ be a Radon measure on $R^d$, which may be non doubling. The only condition that $μ$ must satisfy is $μ(B(x,r))\leq C r^n$, for all $x,r$ and for some fixed $0<n\leq d$. Recently we introduced spaces of type $BMO(μ)$ and $H^1(μ)$ which proved to be useful to study the $L^p(μ)$ boundedness of Calderón-Zygmund operators without assuming doubling conditions. In this paper a characterization of the new atomic space $H^1(μ)$ in terms of a grand maximal operator $M_Φ$ is given. It is shown that $f$ belongs to $H^1(μ)$ iff $f\in L^1(μ)$, $\int f dμ=0$ and $M_Φ(f)\in L^1(μ)$, as in the usual doubling situation. The lack of any regularity condition on $μ$, apart from the size condition stated above, is one of the main difficulties that appears when one tries to extend the classical arguments to the present situation.
dc.description47 pages
dc.identifierhttps://arxiv.org/abs/math/0005060
dc.identifierhttp://arxiv.org/abs/math/0005060
dc.identifier.urihttp://salesiana.dossiersoluciones.com/handle/123456789/59136
dc.subjectClassical Analysis and ODEs
dc.subject42B20 (Primary), 42B30 (Secondary)
dc.titleCharacterization of the atomic space $H^1$ for non doubling measures in terms of a grand maximal operator
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