Weights of Exponential Growth and Decay for Schrödinger-type operators

preprint2020arXivOpen access

Abstract

Fix d≥3d \geq 3 and 1<p<∞1 < p < \infty. Let V:Rd→[0,∞)V : \mathbb{R}^{d} \rightarrow [0,\infty) belong to the reverse Hölder class RHd/2RH_{d/2} and consider the Schrödinger operator LV:=−Δ+VL_{V} := - Δ+ V. In this article, we introduce classes of weights ww for which the Riesz transforms ∇LV−1/2\nabla L_{V}^{-1/2}, their adjoints LV−1/2∇L_{V}^{-1/2} \nabla and the heat maximal operator sup⁡t>0e−tLV∣f∣\sup_{t > 0} e^{- t L_{V}} |f| are bounded on the weighted Lebesgue space Lp(w)L^{p}(w). The boundedness of the LVL_{V}-Riesz potentials LV−α/2L_{V}^{-α/2} from Lp(w)L^{p}(w) to Lν(wν/p)L^ν(w^{ν/p}) for 0<α≤20 < α\leq 2 and 1ν=1p−αd\frac{1}ν = \frac{1}{p} - \fracα{d} will also be proved. These weight classes are strictly larger than a class previously introduced by B. Bongioanni, E. Harboure and O. Salinas that shares these properties and they contain weights of exponential growth and decay. The classes will also be considered in relation to different generalised forms of Schrödinger operator. In particular, the Schrödinger operator with measure potential −Δ+μ- Δ+ μ, the uniformly elliptic operator with potential −divA∇+V- \mathrm{div} A \nabla + V and the magnetic Schrödinger operator (∇−ia)2+V(\nabla - i a)^{2} + V will all be considered. It will be proved that, under suitable conditions, the standard operators corresponding to these second-order differential operators are bounded on Lp(w)L^{p}(w) for weights ww in these classes.

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