Abstract

We study the boundedness of Riesz transforms in $$L^p$$ for $$p>2$$ on a doubling metric measure space endowed with a gradient operator and an injective, $$\omega $$ -accretive operator L satisfying Davies–Gaffney estimates. If L is non-negative self-adjoint, we show that under a reverse Holder inequality, the Riesz transform is always bounded on $$L^p$$ for p in some interval $$[2,2+\epsilon )$$ , and that $$L^p$$ gradient estimates for the semigroup imply boundedness of the Riesz transform in $$L^q$$ for $$q \in [2,p)$$ . This improves results of Auscher et al. (Ann Sci Ecole Norm Sup 37(4):911–957, 2004) and Auscher and Coulhon (Ann Scuola Norm Sup Pisa 4:531–555, 2005), where the stronger assumption of a Poincare inequality and the assumption $$e^{-tL}(1)=1$$ were made. The Poincare inequality assumption is also weakened in the setting of a sectorial operator L. In the last section, we study elliptic perturbations of Riesz transforms.

Highlights

  • The Lp boundedness of Riesz transforms on manifolds has been widely studied in recent years

  • The aim of this article is to give new sufficient criteria for the boundedness of Riesz transforms in Lp for p > 2, and to study its stability under elliptic perturbations

  • We introduce a property (RHp), which describes a reverse local Holder inequality for the gradient of harmonic functions

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Summary

Introduction

The Lp boundedness of Riesz transforms on manifolds has been widely studied in recent years. We introduce a property (RHp) (see Definition 2.8), which describes a reverse local Holder inequality for the gradient of harmonic functions This property already appeared in [27] for the solutions of elliptic PDEs. In the context of Riesz transform bounds, it was already used in various results for Schrodinger operators [40, 5, 39], and in [6] for the Laplace-Beltrami operator on a Riemannian manifold. It is unknown if (Gp) together with (Pp) implies (P2) The proof of this statement in [12, Theorem 6.3] relies on the self-adjointness of the operator, which is used through the finite propagation speed property to deduce a perfectly localised Caccioppoli inequality. Let us state a technical result, which describes how a higher order of cancellation with respect to the operator L allows us to gain integrability through off-diagonal estimates

Then for every ball of radius r
This gives for ρ
Then by
Suppose in addition every f
An analogous computation yields
Br p
Therefore yields
So we have
Since pL ν and
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