中文

双参数Littlewood-Paley算子在乘积Hardy空间上的有界性

经典分析与常微分方程 2016-05-03 v1

摘要

n1,n21,λ1>1n_1,n_2\ge 1, \lambda_1>1λ2>1\lambda_2>1。对于任意 x=(x1,x2)Rn×Rmx=(x_1,x_2) \in \mathbb {R}^n\times\mathbb{R}^m,令 gggλg_{\vec{\lambda}}^* 为由以下定义的双参数Littlewood-Paley平方函数 \begin{align*} g(f)(x)= \Big(\int_0^{\infty}\int_0^{\infty}|\theta_{t_1,t_2} f(x_1,x_2)|^2 \frac{dt_1}{t_1} \frac{dt_2}{t_2} \Big)^{1/2}, \hbox{and} \end{align*} gλ(f)(x)=(R+m+1R+n+1i=12(t1ti+xiyi)niλiθt1,t2f(y1,y2)2dy1dt1t1n+1dy2dt2t2m+1)1/2, g_{\vec{\lambda}}^*(f)(x) = \Big(\iint_{\mathbb{R}^{m+1}_{+}} \iint_{\mathbb{R}^{n+1}_{+}} \prod_{i=1}^2\Big(\frac{t_1}{t_i + |x_i - y_i|}\Big)^{n_i \lambda_i} |\theta_{t_1,t_2} f(y_1,y_2)|^2 \frac{dy_1 dt_1}{t_1^{n+1}} \frac{dy_2 dt_2}{t_2^{m+1}} \Big)^{1/2}, \noindent 其中 θt1,t2f(x1,x2)=Rn×Rmst1,t2(x1,x2,y1,y2)f(y1,y2)dy1dy2\theta_{t_1,t_2} f(x_1, x_2) = \iint_{\mathbb{R}^n\times\mathbb{R}^m} s_{t_1,t_2}(x_1,x_2,y_1,y_2)f(y_1,y_2) dy_1dy_2。已知双参数 gggλg_{\vec{\lambda}}^*L2L^2 有界性最近已由Martikainen和Cao、Xue分别建立。本文中,在对核 st1,t2s_{t_1,t_2} 假设特定结构条件下,我们证明 gggλg_{\vec{\lambda}}^* 均从乘积Hardy空间 H1(Rn×Rm)H^1(\mathbb{R}^n\times\mathbb{R}^m)L1(Rn×Rm)L^1(\mathbb{R}^n\times\mathbb{R}^m) 有界。作为推论,将得到 gggλg_{\vec{\lambda}}^*1<p<21<p<2 时的 LpL^p 有界性。

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引用

@article{arxiv.1605.00476,
  title  = {Boundedness of Bi-parameter Littlewood-Paley operators on product Hardy space},
  author = {Zhengyang Li and Qingying Xue},
  journal= {arXiv preprint arXiv:1605.00476},
  year   = {2016}
}

备注

26 pages