2011/07/17 by Dachun Yang, Yang, Dachun, Sibei Yang +1
Mathematics · #35J25 #42B20 #42B25 #42B37 #47B38 #Advanced Harmonic Analysis Research #Classical Analysis and ODEs (math.CA) #FOS: Mathematics #Functional Analysis (math.FA) #Holomorphic and Operator Theory #Nonlinear Partial Differential Equations #Primary: 42B30 #Secondary: 42B35 #math.CA #math.FA #msc:35J25 #msc:42B20 #msc:42B25 #msc:42B30 #msc:42B35 #msc:42B37 #msc:47B38
paper · pdf · doi:10.48550/arxiv.1107.3267
65 pages, Rev. Mat. Iberoam. (to appear)
arxiv created 2011/07/17 · openalex publication_date 2011/07/17 · arxiv updated 2011/07/19 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
Let Ω be a strongly Lipschitz domain of ℝn, whose complement in ℝn is unbounded. Let L be a second order divergence form elliptic operator on L2 (Ω) with the Dirichlet boundary condition, and the heat semigroup generated by L have the Gaussian property (Gdiam(Ω)) with the regularity of their kernels measured by μ∈(0,1], where diam(Ω) denotes the diameter of Ω. Let Φ be a continuous, strictly increasing, subadditive and positive function on (0,∞) of upper type 1 and of strictly critical lower type pΦ∈(n/(n+μ),1]. In this paper, the authors introduce the Orlicz-Hardy space HΦ, r(Ω) by restricting arbitrary elements of the Orlicz-Hardy space HΦ(ℝn) to \boz and establish its atomic decomposition by means of the Lusin area function associated with \e-tL\t≥0. Applying this, the authors obtain two equivalent characterizations of HΦ, r(\boz) in terms of the nontangential maximal function and the Lusin area function associated with the heat semigroup generated by L.