Abstract

AbstractThe main part of this paper is a shorter version of a joint work with P. Sjögren. Let G be the Lie group ℝ2⋊ℝ+ endowed with the Riemannian symmetric space structure. Let X 0, X 1, X 2 be a distinguished basis of left-invariant vector fields of the Lie algebra of G and define the Laplacian \(\varDelta=-(X_{0}^{2}+X_{1}^{2}+X_{2}^{2})\). We recall the definition and the main properties of the atomic Hardy space \(H^{1}_{\mathrm{at}}\) introduced on the group G in a previous paper of the author. Then we introduce a maximal Hardy space \(H^{1}_{\mathrm{max},\mathrm{h}}\) on G defined in terms of the maximal function associated with the heat kernel of the Laplacian Δ. We show that the atomic Hardy space is strictly included in the heat maximal Hardy space. In the last part of the paper, which is new, we consider the maximal Hardy space \(H^{1}_{\mathrm{max},\mathrm{p}}\) defined in terms of the Poisson kernel of the Laplacian Δ and show that it strictly contains the atomic Hardy space \(H^{1}_{\mathrm{at}}\).KeywordsHeat kernelMaximal functionHardy spaceLie groupsExponential growthMathematics Subject Classification (2010)22E3042B3035K0842B25

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