2011/06/24 by Chin-Cheng Lin, Lin, Chin-Cheng, Heping Liu +3
Mathematics · #Advanced Harmonic Analysis Research #Advanced Mathematical Physics Problems #Analysis of PDEs (math.AP) #FOS: Mathematics #Mathematical Analysis and Transform Methods
paper · pdf · doi:10.48550/arxiv.1106.4960
openalex publication_date 2011/06/24 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28
Let L= -Δℍn+V be a Schrödinger operator on the Heisenberg group ℍn, where Δℍn is the sub-Laplacian and the nonnegative potential V belongs to the reverse Hölder class B(Q)/(2) and Q is the homogeneous dimension of ℍn. The Riesz transforms associated with the Schrödinger operator L are bounded from L1(ℍn) to L1,∞(ℍn). The L1 integrability of the Riesz transforms associated with L characterizes a certain Hardy type space denoted by H1L(ℍn) which is larger than the usual Hardy space H1(ℍn). We define H1L(ℍn) in terms of the maximal function with respect to the semigroup \e-s L: s>0 \, and give the atomic decomposition of H1L(ℍn). As an application of the atomic decomposition theorem, we prove that H1L(ℍn) can be characterized by the Riesz transforms associated with L. All results hold for stratified groups as well.