q 变霍尔曼德函数微积分与薛定谔和波最大估计

IF 1 3区 数学 Q1 MATHEMATICS Mathematische Zeitschrift Pub Date : 2024-05-02 DOI:10.1007/s00209-024-03488-7
Luc Deleaval, Christoph Kriegler
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引用次数: 0

摘要

本文是 [30] 工作的继续,在 [30] 中我们证明了最大估计值 $$\begin{aligned}\left\| \sup _{t >;0} |m(tA)f| \, \right\| _{L^p(\Omega ,Y)} \leqslant C \left\| f\right\| _{L^p(\Omega ,Y)} \end{aligned}$$ 对于作用在 \(L^p(\Omega 、Y)上作用的扇形算子 A(Y 是一个 UMD 网格),并且允许一个 Hörmander 函数微积分(全态 \(H^\infty)微积分的加强,以量化的方式在 \((0,\infty )上可微分的符号 m),以及 \(m :(0, \infty ) rightarrow \mathbb {C}\) 是在\(\infty \)有一定衰减的霍曼德类符号。在本文中,我们证明了在上述相同条件下,标量函数 \(t \mapsto m(tA)f(x,\omega )\) 是有限q变的,即 \((x,\omega )\) 。这扩展了[13, 44,45,46, 52, 61]最近的工作,他们考虑了\(m(tA) = e^{-tA}\) 所产生的半群。因此,我们将 [52] 中对欧几里得空间中球面均值的估计扩展到了 UMD 格值空间的情形。第二个主要结果产生了一个最大估计 $$\begin{aligned}\left\| \sup _{t > 0} |m(tA) f_t| \, \right\| _{L^p(\Omega ,Y)} \leqslant C \left\| f_t\right\| _{L^p(\Omega ,Y(\Lambda ^\beta ))}\end{aligned}$$对于上面相同的 A 和类似的 m 条件,但是 \(f_t\) 本身依赖于 t,这样 \(t \mapsto f_t(x,\omega )\) 属于一个 Sobolev 空间 \(\Lambda ^\beta \) over \((\mathbb {R}_+, \frac{dt}{t})\)。我们以此来展示薛定谔(A = -\Delta \)或波(A = \sqrt{-\Delta })解传播者\(t \mapsto \exp (itA)f\) 的最大估计值。然后我们从中推导出卡莱森点式收敛问题变体的解[18] $$\begin{aligned}\ext { a. e. }(x,\omega ) \quad (t \rightarrow 0+) \end{aligned}$$对于 A 一个傅立叶乘法算子或一个具有边界条件的开放域 \(\Omega \subseteq \mathbb {R}^d\)上的微分算子。
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q-variational Hörmander functional calculus and Schrödinger and wave maximal estimates

This article is the continuation of the work [30] where we had proved maximal estimates

$$\begin{aligned} \left\| \sup _{t > 0} |m(tA)f| \, \right\| _{L^p(\Omega ,Y)} \leqslant C \left\| f\right\| _{L^p(\Omega ,Y)} \end{aligned}$$

for sectorial operators A acting on \(L^p(\Omega ,Y)\) (Y being a UMD lattice) and admitting a Hörmander functional calculus (a strengthening of the holomorphic \(H^\infty \) calculus to symbols m differentiable on \((0,\infty )\) in a quantified manner), and \(m : (0, \infty ) \rightarrow \mathbb {C}\) being a Hörmander class symbol with certain decay at \(\infty \). In the present article, we show that under the same conditions as above, the scalar function \(t \mapsto m(tA)f(x,\omega )\) is of finite q-variation with \(q > 2\), a.e. \((x,\omega )\). This extends recent works by [13, 44,45,46, 52, 61] who have considered among others \(m(tA) = e^{-tA}\) the semigroup generated by \(-A\). As a consequence, we extend estimates for spherical means in euclidean space from [52] to the case of UMD lattice-valued spaces. A second main result yields a maximal estimate

$$\begin{aligned} \left\| \sup _{t > 0} |m(tA) f_t| \, \right\| _{L^p(\Omega ,Y)} \leqslant C \left\| f_t\right\| _{L^p(\Omega ,Y(\Lambda ^\beta ))} \end{aligned}$$

for the same A and similar conditions on m as above but with \(f_t\) depending itself on t such that \(t \mapsto f_t(x,\omega )\) belongs to a Sobolev space \(\Lambda ^\beta \) over \((\mathbb {R}_+, \frac{dt}{t})\). We apply this to show a maximal estimate of the Schrödinger (case \(A = -\Delta \)) or wave (case \(A = \sqrt{-\Delta }\)) solution propagator \(t \mapsto \exp (itA)f\). Then we deduce from it solutions to variants of Carleson’s problem of pointwise convergence [18]

$$\begin{aligned} \exp (itA)f(x,\omega ) \rightarrow f(x,\omega ) \text { a. e. }(x,\omega ) \quad (t \rightarrow 0+) \end{aligned}$$

for A a Fourier multiplier operator or a differential operator on an open domain \(\Omega \subseteq \mathbb {R}^d\) with boundary conditions.

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1.60
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236
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3-6 weeks
期刊介绍: "Mathematische Zeitschrift" is devoted to pure and applied mathematics. Reviews, problems etc. will not be published.
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