Boundedness of Bi-parameter Littlewood-Paley operators on product Hardy space

preprint2016arXivOpen access

Abstract

Let n1,n2≥1,λ1>1n_1,n_2\ge 1, λ_1>1 and λ2>1λ_2>1. For any x=(x1,x2)∈Rn×Rmx=(x_1,x_2) \in \mathbb {R}^n\times\mathbb{R}^m, let gg and gλ⃗∗g_{\vecλ}^* be the bi-parameter Littlewood-Paley square functions defined by \begin{align*} g(f)(x)= \Big(\int_0^{\infty}\int_0^{\infty}|θ_{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*} gλ⃗∗(f)(x)=(∬R+m+1∬R+n+1∏i=12(t1ti+∣xi−yi∣)niλi∣θt1,t2f(y1,y2)∣2dy1dt1t1n+1dy2dt2t2m+1)1/2, g_{\vecλ}^*(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 λ_i} |θ_{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 where θt1,t2f(x1,x2)=∬Rn×Rmst1,t2(x1,x2,y1,y2)f(y1,y2)dy1dy2θ_{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. It is known that the L2L^2 boundedness of bi-parameter gg and gλ⃗∗g_{\vecλ}^* have been established recently by Martikainen, and Cao, Xue, respectively. In this paper, under certain structure conditions assumed on the kernel st1,t2,s_{t_1,t_2}, we show that both gg and gλ⃗∗g_{\vecλ}^* are bounded from product Hardy space H1(Rn×Rm)H^1(\mathbb{R}^n\times\mathbb{R}^m) to L1(Rn×Rm)L^1(\mathbb{R}^n\times\mathbb{R}^m). As consequences, the LpL^p boundedness of gg and gλ⃗∗g_{\vecλ}^* will be obtained for 1<p<21<p<2.

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