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Endpoint boundedness of singular integrals: CMO space associated to Schrödinger operators

Xueting Han, Ji Li, Liangchuan Wu

TL;DR

This work studies endpoint boundedness for classical singular integrals on the Schrödinger-operator- adapted vanishing mean oscillation space ${\rm CMO}_{\mathcal L}(\mathbb{R}^n)$ with ${\mathcal L}=-\Delta+V$ and $V\in RH_q$, $q\ge \frac{n}{2}$. The authors establish three main results: (i) the Hardy-Littlewood maximal operator $M$ is bounded on ${\rm CMO}_{\mathcal L}$, (ii) the adjoint Riesz transforms $R_j^*$ map $C_0(\mathbb{R}^n)$ into ${\rm CMO}_{\mathcal L}$, and (iii) the Poisson and heat semigroup–driven approximations to the identity characterize ${\rm CMO}_{\mathcal L}$. The proofs rely on sharp heat-kernel estimates and the tent-space framework for ${\rm CMO}_{\mathcal L}$, rather than classical Calderón–Zygmund theory, and yield a Riesz-type representation for functionals on ${\rm CMO}_{\mathcal L}$. When $V\equiv0$, these results recover the classical ${\rm CMO}$ theory, illustrating how the potential complicates the analysis yet preserves a parallel structure. The findings have implications for harmonic analysis in Schrödinger settings and for associated function-space dualities.

Abstract

Let $ \mathcal{L} = -Δ+ V $ be a Schrödinger operator acting on $ L^2(\mathbb{R}^n) $, where the nonnegative potential $ V $ belongs to the reverse Hölder class $ RH_q $ for some $ q \geq n/2 $. This article is primarily concerned with the study of endpoint boundedness for classical singular integral operators in the context of the space $ \mathrm{CMO}_{\mathcal{L}}(\mathbb{R}^n) $, consisting of functions of vanishing mean oscillation associated with $ \mathcal{L} $. We establish the following main results: (i) the standard Hardy--Littlewood maximal operator is bounded on $\mathrm{CMO}_{\mathcal{L}}(\mathbb{R}^n) $; (ii) for each $ j = 1, \ldots, n$, the adjoint of the Riesz transform $ \partial_j \mathcal{L}^{-1/2} $ is bounded from $ C_0(\mathbb{R}^n) $ into $ \mathrm{CMO}_{\mathcal{L}}(\mathbb{R}^n) $; and (iii) the approximation to the identity generated by the Poisson and heat semigroups associated with $ \mathcal{L} $ characterizes $ \mathrm{CMO}_{\mathcal{L}}(\mathbb{R}^n) $ appropriately. These results recover the classical analogues corresponding to the Laplacian as a special case. However, the presence of the potential $ V $ introduces substantial analytical challenges, necessitating tools beyond the scope of classical Calderón--Zygmund theory. Our approach leverages precise heat kernel estimates and the structural properties of $ \mathrm{CMO}_{\mathcal{L}}(\mathbb{R}^n) $ established by Song and the third author in [J. Geom. Anal. 32 (2022), no. 4, Paper No. 130, 37 pp].

Endpoint boundedness of singular integrals: CMO space associated to Schrödinger operators

TL;DR

This work studies endpoint boundedness for classical singular integrals on the Schrödinger-operator- adapted vanishing mean oscillation space with and , . The authors establish three main results: (i) the Hardy-Littlewood maximal operator is bounded on , (ii) the adjoint Riesz transforms map into , and (iii) the Poisson and heat semigroup–driven approximations to the identity characterize . The proofs rely on sharp heat-kernel estimates and the tent-space framework for , rather than classical Calderón–Zygmund theory, and yield a Riesz-type representation for functionals on . When , these results recover the classical theory, illustrating how the potential complicates the analysis yet preserves a parallel structure. The findings have implications for harmonic analysis in Schrödinger settings and for associated function-space dualities.

Abstract

Let be a Schrödinger operator acting on , where the nonnegative potential belongs to the reverse Hölder class for some . This article is primarily concerned with the study of endpoint boundedness for classical singular integral operators in the context of the space , consisting of functions of vanishing mean oscillation associated with . We establish the following main results: (i) the standard Hardy--Littlewood maximal operator is bounded on ; (ii) for each , the adjoint of the Riesz transform is bounded from into ; and (iii) the approximation to the identity generated by the Poisson and heat semigroups associated with characterizes appropriately. These results recover the classical analogues corresponding to the Laplacian as a special case. However, the presence of the potential introduces substantial analytical challenges, necessitating tools beyond the scope of classical Calderón--Zygmund theory. Our approach leverages precise heat kernel estimates and the structural properties of established by Song and the third author in [J. Geom. Anal. 32 (2022), no. 4, Paper No. 130, 37 pp].

Paper Structure

This paper contains 5 sections, 8 theorems, 146 equations, 1 figure.

Key Result

Theorem 1.1

Suppose $V\in RH_q$ for some $q\geq n/2$ and let $\mathcal{L}=-\Delta+V$. For each $f\in {\rm BMO}_{\mathcal{L}}(\mathbb R^n)$, the Hardy--Littlewood maximal function $Mf$ belongs to ${\rm BMO}_{\mathcal{L}}(\mathbb R^n)$ as well, with where the constant $C>0$ is independent of $f$. Moreover, if $f\in {\rm CMO}_{\mathcal{L}}(\mathbb R^n)$, we also have $Mf\in {\rm CMO}_{\mathcal{L}}(\mathbb R^n)

Figures (1)

  • Figure 1: $Q"$ contains $Q$ and $Q'$, and shares a common vertex with $Q'$.

Theorems & Definitions (20)

  • Theorem 1.1
  • Theorem 1.2
  • Theorem 1.3
  • Theorem 2.1
  • Lemma 2.2
  • proof : Proof of Theorem \ref{['thm:M-CMO']}
  • Remark 3.1
  • Remark 3.2
  • proof : Proof of Theorem \ref{['thm:Riesz-CMO']}
  • Lemma 4.1
  • ...and 10 more