Abstract:Abstract. Let M be a complete connected Riemannian manifold. Assuming that the Riemannian measure is doubling, we define Hardy spaces H p of differential forms on M and give various characterizations of them, including an atomic decomposition. As a consequence, we derive the H p -boundedness for Riesz transforms on M, generalizing previously known results. Further applications, in particular to H ∞ functional calculus and Hodge decomposition, are given.
“…follows from [AMR,Theorem 5.13] and that of the imaginary powers from [DY,Corollary 4.3]. However, we believe that the proofs outlined here might be of some interest for their simplicity.…”
Abstract. In this paper we consider a complete connected noncompact Riemannian manifold M with bounded geometry and spectral gap. We prove that the imaginary powers of the Laplacian and the Riesz transform are bounded from the Hardy space X 1 (M ), introduced in previous work of the authors, to
“…follows from [AMR,Theorem 5.13] and that of the imaginary powers from [DY,Corollary 4.3]. However, we believe that the proofs outlined here might be of some interest for their simplicity.…”
Abstract. In this paper we consider a complete connected noncompact Riemannian manifold M with bounded geometry and spectral gap. We prove that the imaginary powers of the Laplacian and the Riesz transform are bounded from the Hardy space X 1 (M ), introduced in previous work of the authors, to
“…In this case, we can choose b (3) and a (4) to be any positive number. For example, we let b (3) = b (1) and a (4) = a (2) . (4) and a (5) be any positive number.…”
Section: Lemma 42 Fix X ∈ O I the Properties Of The Set Defining mentioning
confidence: 99%
“…For the theory of Hardy spaces associated to operators, it has attracted a lot of attention in the last decades, and has been a very active research topic in harmonic analysis -see for example, [1,2,3,7,10,11,12,13,15,16,17,18,21,23,24].…”
Section: Introductionmentioning
confidence: 99%
“…We now recall the notion of a (p, q, M)-atom associated to an operator L ( [2,11,15]). The atomic Hardy space H p L,at,q,M (X) is defined as follows.…”
Abstract. Let X be a metric measure space with a doubling measure and L be a nonnegative selfadjoint operator acting on L 2 (X). Assume that L generates an analytic semigroup e −tL whose kernels p t (x, y) satisfy Gaussian upper bounds but without any assumptions on the regularity of space variables x and y. In this article we continue a study in [21] to give an atomic decomposition for the Hardy spaces H p L,max (X) in terms of the nontangential maximal function associated with the heat semigroup of L, and hence we establish characterizations of Hardy spaces associated to an operator L, via an atomic decomposition or the nontangential maximal function. We also obtain an equivalence of H p L,max (X) in terms of the radial maximal function.
“…Yang and his cooperators discussed new Orlicz-Hardy spaces associated with operators [10][11][12][13]. For more results, we refer to [14][15][16][17][18][19] and the references therein.…”
Suppose is a nonnegative, self-adjoint differential operator. In this paper, we introduce the Herz-type Hardy spaces associated with operator . Then, similar to the atomic and molecular decompositions of classical Herz-type Hardy spaces and the Hardy space associated with operators, we prove the atomic and molecular decompositions of the Herz-type Hardy spaces associated with operator . As applications, the boundedness of some singular integral operators on Herz-type Hardy spaces associated with operators is obtained.
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