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Carleson measures, BMO spaces and balayages associated to Schrödinger operators

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Abstract

Let L be a Schrödinger operator of the form L = −Δ+V acting on L 2(Rn), n ≥ 3, where the nonnegative potential V belongs to the reverse Hölder class B q for some qn: Let BMOL(Rn) denote the BMO space associated to the Schrödinger operator L on Rn. In this article, we show that for every f ∈ BMOL(Rn) with compact support, then there exist g ∈ L∞(Rn) and a finite Carleson measure μ such that

$$f\left( x \right) = g\left( x \right) + {S_{\mu ,}}_P\left( x \right)$$

with \({\left\| g \right\|_\infty } + |||\mu ||{|_c} \leqslant C{\left\| f \right\|_{BM{O_L}\left( {{\mathbb{R}^n}} \right)}}\); where

$${S_{\mu ,P}} = \int_{\mathbb{R}_ + ^{n + 1}} {{P_t}\left( {x,y} \right)d\mu \left( {y,t} \right)} $$

, and P t (x; y) is the kernel of the Poisson semigroup \(\left\{ {{e^{ - t\sqrt L }}} \right\}t > 0\) on L 2(Rn). Conversely, if μ is a Carleson measure, then S μ;P belongs to the space BMOL(Rn). This extends the result for the classical John-Nirenberg BMO space by Carleson (1976) (see also Garnett and Jones (1982), Uchiyama (1980) and Wilson (1988)) to the BMO setting associated to Schrödinger operators.

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Acknowledgements

This work was supported by National Natural Science Foundation of China (Grant Nos. 11501583, 11471338, 11622113, 11371378 and 11521101), Australian Research Council Discovery (Grant Nos. DP 140100649 and DP 170101060), Guangdong Natural Science Funds for Distinguished Young Scholar (Grant No. 2016A030306040) and Guangdong Special Support Program. The fifth author thanks J. Michael Wilson for helpful discussions.

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Correspondence to LiXin Yan.

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In memory of the 100th birthday of CHENG MinDe

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Chen, P., Duong, X.T., Li, J. et al. Carleson measures, BMO spaces and balayages associated to Schrödinger operators. Sci. China Math. 60, 2077–2092 (2017). https://doi.org/10.1007/s11425-016-9147-y

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  • DOI: https://doi.org/10.1007/s11425-016-9147-y

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