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数学物理学报, 2023, 43(1): 1-13

\boldsymbol{H^{p,q,s}}({\Bbb D})上的复合算子

陈洪欣,, 张学军,*, 周敏,

湖南师范大学数学与统计学院 长沙410006

Composition Operators on \boldsymbol{H^{p,q,s}}({\Bbb D})

Chen Hongxin,, Zhang Xuejun,*, Zhou Min,

College of Mathematics and Statistics, Hunan Normal University, Changsha 410006

通讯作者: *张学军, E-mail: xuejunttt@263.net

收稿日期: 2022-05-2   修回日期: 2022-08-5  

基金资助: 国家自然科学基金(11942109)
湖南省自然科学基金(2022JJ30369)

Received: 2022-05-2   Revised: 2022-08-5  

Fund supported: The NSFC(11942109)
The NSFH(2022JJ30369)

作者简介 About authors

陈洪欣,E-mail:1755310775@qq.com

周敏,E-mail:1479898554@qq.com

摘要

\varphi 是复平面{\Bbb C}中单位圆盘 {\Bbb D}上的解析自映射. 该文刻画了一般Hardy型空间H^{p,q,s}({\Bbb D})上使得复合算子C_{\varphi}有界或者紧时的符号函数 \varphi.

关键词: 复合算子; 有界性; 紧性; 一般 Hardy 型空间; 单位圆盘

Abstract

Let \varphi be an analytic self-map of the unit disc {\Bbb D} in the complex plane {\Bbb C}. In this paper, the authors characterize those symbols \varphi such that composition operators C_{\varphi} are bounded or compact on the general Hardy type space H^{p,q,s}({\Bbb D}).

Keywords: Composition operator; Boundedness; Compactness; General Hardy type space; Unit disc

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本文引用格式

陈洪欣, 张学军, 周敏. \boldsymbol{H^{p,q,s}}({\Bbb D})上的复合算子[J]. 数学物理学报, 2023, 43(1): 1-13

Chen Hongxin, Zhang Xuejun, Zhou Min. Composition Operators on \boldsymbol{H^{p,q,s}}({\Bbb D})[J]. Acta Mathematica Scientia, 2023, 43(1): 1-13

1 引言

{\Bbb D} 是复平面 {\Bbb C}上的单位圆盘, H({\Bbb D}) 表示 {\Bbb D}上的解析函数类, H^{\infty}({\Bbb D}) 表示 {\Bbb D} 上的有界解析函数空间. 首先, 我们介绍几个本文要涉及的函数空间.

定义 1.1p>0, 若 h\in H({\Bbb D})且满足

\| h\| _{p}=\sup_{u\in {\Bbb D}}(1-|u|^{2})^{p}\ | h(u)|<\infty,

则称h属于增长空间 H^{\infty}_{p}({\Bbb D}).

定义 1.2p>0q> 0, 若 h\in H({\Bbb D})且满足

\| h\| _{p,q}=\sup_{0\leq r<1}\left\{(1-r^{2})^{q}\int_{0}^{2\pi}|h(r{\rm e}^{{\rm i}\theta})|^{p}\ \frac{{\rm d}\theta}{2\pi}\right\}^{\frac{1}{p}}<\infty,

则称h属于加权 Hardy 空间 H_{q}^{p}({\Bbb D}).

定义 1.3\beta>-1p>0, 若 h\in H({\Bbb D})且满足

\| h\| _{A_{\beta}^{p}}=\left(\int_{{\Bbb D}}|h(u)|^{p}\ {\rm d}v_{\beta}(u)\right)^{\frac{1}{p}}<\infty,

则称h属于加权 Bergman 空间 A_{\beta}^{p}({\Bbb D}), 其中 {\rm d}v{\Bbb D}上正规化 Lebesgue 测度且 {\rm d}v_{\beta}(u)=(\beta+1)(1-|u|^{2})^{\beta}\ {\rm d}v(u).

给定 w\in {\Bbb D}, 设 {\Bbb D}上的解析自同构 \varphi_{w}(z)=\frac{w-z}{1-\overline{w}z}, 很容易验证 \varphi_{w} 满足 \varphi_{w}(0) = w\varphi_{w}(w)=0以及 \varphi_{w}^{-1}=\varphi_{w}.

定义 1.4p>0, q+1\geq 0, s\geq 0, q+s\geq 0, 若 h\in H({\Bbb D}) 且满足

\| h\| _{p,q,s}=\sup_{0\leq \rho<1}M_{p,q,s}(\rho,h)<\infty,

则称 h 属于一般Hardy型空间 H^{p,q,s}({\Bbb D}), 其中

M_{p,q,s}^{p}(\rho,h)=\sup_{w\in {\Bbb D}}(1-\rho^{2})^{q}\int_{0}^{2\pi}|h(\rho {\rm e}^{{\rm i}\theta})|^{p}\ (1-|\varphi_{w}(\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}\ \frac{{\rm d}\theta}{2\pi}.

p\geq 1 时, H^{p,q,s}({\Bbb D}) 依范数 \|\cdot \| _{p,q,s} 构成一个Banach空间; 当 0<p<1 时, H^{p,q,s}({\Bbb D}) 依距离 r(h,g)=\| h-g\| ^{p}_{p,q,s} 构成一个完备的距离空间. 特别地, 当 q=s=0 时, H^{p,q,s}({\Bbb D}) 恰好是 Hardy 空间H^{p}({\Bbb D}). 因此, H^{p,q,s}({\Bbb D}) 是 Hardy 空间 H^{p}({\Bbb D}) 的一种推广. 空间 H^{p,q,s}({\Bbb D}) 来源于一些实际应用[1-3], 并在文献[4]中被正式命名为单位球上一般 Hardy 型空间. 最近, 我们在文献[5,6]中进一步讨论了该空间的一些性质. 实际上, H^{p,q,s}({\Bbb D}) 含有几个经典函数空间, 例如, 当 s\geq 1=-q 时, H^{p,q,s}({\Bbb D})= H^{\infty}({\Bbb D}), 当 s\geq 1>-q 时, H^{p,q,s}({\Bbb D})=H^{\infty}_{\frac{q+1}{p}}({\Bbb D}), 当 q>0=s 时, H^{p,q,s}({\Bbb D})=H^{p}_{q}({\Bbb D}).0<s<1 时, H^{p,q,s}({\Bbb D}) 是一个不同于Hardy 空间 H^{k}({\Bbb D}) ( 0<k\leq \infty) 和加权Hardy 空间 H^{k}_{t}({\Bbb D}) (0<t<\infty) 的新函数空间 (可参见文献[5]).

定义 1.5\varphi: {\Bbb D}\rightarrow {\Bbb D} 是一个解析映射, \varphi 诱导H({\Bbb D}) 上一个算子C_{\varphi}: C_{\varphi}g=g\circ\varphi, 称该算子 C_{\varphi} 为复合算子.

单位圆盘或单位球上各种解析函数之间复合型算子的研究已经具有相当长的历史, 并且有了大量的研究成果, 其中与本文有直接关系的文献如 [1-3,7-17] 等. 本文的主要目的就是讨论 H^{p,q,s}({\Bbb D})上复合算子 C_{\varphi} 有界或紧时符号函数 \varphi 满足的条件.

本文中,若存在常数 c>0 使得 E_{1} \geq cE_{2} (或 E_{1} \leq cE_{2}), 我们记为 "E_{1} \gtrsim E_{2}" (或 "E_{1}\lesssim E_{2}")."E_{1} \gtrsim E_{2}" "E_{1}\lesssim E_{2}", 称 E_{1}E_{2} 等价, 记为 "E_{1}\asymp E_{2}".

2 一些引理

引理 2.1[5]h\in H^{p,q,s}({\Bbb D}), 则

|h(z)|\lesssim\frac{\| h\| _{p,q,s}}{(1-|z|^{2})^{\frac{q+1}{p}}} \ \ \mbox{对所有 $z\in {\Bbb D}$ 成立}.

引理 2.2[9]\beta>-1, 若 h\in A_{\beta}^{1}({\Bbb D}), 则可由积分表示

h(z)=\int_{{\Bbb D}}\frac{h(w) \ {\rm d}v_{\beta}(w)}{(1-z \overline{w})^{2+\beta}} \ \ (z\in {\Bbb D}).

引理 2.3[10]c>0\delta>-1, 则

\int_{0}^{2\pi}\frac{{\rm d}\theta}{|1-\overline{w} {\rm e}^{{\rm i}\theta}|^{1+c}}\asymp \int_{{\Bbb D}}\frac{(1-|u|^{2})^{\delta}\ {\rm d}v(u)}{|1-\overline{w}u|^{2+\delta+c}}\asymp\frac{1}{(1-|w|^{2})^{c}} \ \ \mbox{对所有 $w\in {\Bbb D}$ 成立}.

下列引理是 Littlewood 从属定理 (可参见文献[12]).

引理 2.4[12]p>0 以及 \psi:{\Bbb D}\rightarrow {\Bbb D} 是一个解析映射且满足 \psi(0)=0, 则

\int_{0}^{2\pi}|f[\psi(\rho {\rm e}^{{\rm i}\theta})]|^{p}\ {\rm d}\theta\leq \int_{0}^{2\pi}|f(\rho {\rm e}^{{\rm i}\theta})|^{p}\ {\rm d}\theta

对所有 f\in H({\Bbb D})0\leq \rho<1 成立.

{\Bbb D}内两点有下列积分双向估计. 这些结果来自文献[4]中命题3.1 (情形 n=1).

引理 2.5[4]wa {\Bbb D} 中两点.对 r> 0t> 0, 记

I_{w,a}=\int_{0}^{2\pi}\frac{{\rm d}\theta}{|1-\overline{w}{\rm e}^{{\rm i}\theta}|^{ t}\ |1-\overline{a}{\rm e}^{{\rm i}\theta}|^{ r}},

则有下列双向估计

(1) 当 t+r>1\max\{t,r\}<1 时, I_{w,a}\asymp \frac{1}{ |1-w\overline{a}|^{t+r-1}}.

(2) 当 t=1>r 时, I_{w,a}\asymp\frac{1}{|1-w\overline{a}|^{r}}\log\frac{e}{|1-w\overline{\varphi_{w}(a)}|}.

(3) 当 t=1=r 时, I_{w,a}\asymp \frac{1}{|1-w\overline{a}|}\log\frac{e}{1-|\varphi_{w}(a)|^{2}}.

(4) 当 t>1>r 时, I_{w,a}\asymp \frac{1}{(1-|w|^{2})^{ t-1}\ |1-w\overline{a}|^{ r}}.

(5) 当 t>1r>1 时, I_{w,a} \asymp\frac{1}{(1-|w|^{2})^{t-1}|1-w\overline{a}|^{ r}} + \frac{1}{(1-|a|^{2})^{ r-1}|1-w\overline{a}|^{ t}}.

(6) 当 t>1=r 时, I_{w,a} \asymp \frac{1}{(1-|w|^{2})^{t-1}|1-w\overline{a}|} + \frac{1}{|1-w\overline{a}|^{ t}}\log\frac{e}{1-|\varphi_{a}(w)|^{2}}.

引理 2.6[6]p>00<p_{0}\leq 1, 则

(1-\rho^{2})^{\frac{1-p_{0}}{p_{0}}}\int_{0}^{2\pi}|h(\rho^{2}{\rm e}^{{\rm i}\theta})|^{p}\ {\rm d}\theta\leq \left\{\int_{0}^{2\pi}|h(\rho {\rm e}^{{\rm i}\tau})|^{pp_{0}}\ {\rm d}\tau\right\}^{\frac{1}{p_{0}}}

对所有 h\in H({\Bbb D})0\leq \rho<1 成立.

3 主要结果

定理 3.1\varphi: \ {\Bbb D}\rightarrow {\Bbb D} 是一个解析映射.

(1) 若 \varphi 是一个自同构, 则 C_{\varphi}H^{p,q,s}({\Bbb D}) 上有界.

(2) 若 s\geq 1\geq -qs=0\leq q, 则 C_{\varphi}H^{p,q,s}({\Bbb D}) 上总是有界的.

(3) 若 q+1>0C_{\varphi}H^{p,q,s}({\Bbb D}) 上的紧算子, 则

\lim_{|w|\rightarrow 1^{-}}\frac{1-|w|^{2}}{1-|\varphi(w)|^{2}}=0.
(3.1)

(4) 若 s\geq 1> -qs=0< q, 则 C_{\varphi}H^{p,q,s}({\Bbb D}) 上紧当且仅当(3.1)式成立.

(5) 若 q=0=s, 则 C_{\varphi}H^{p,q,s}({\Bbb D}) 上的紧算子当且仅当

\lim_{|w|\rightarrow 1^{-}}\frac{N_{\varphi}(w)}{1-|w|^{2}}=0,
(3.2)

其中 N_{\varphi}(w) 是计数函数.

(6) 若 \| \varphi\| _{\infty}<1, 则 C_{\varphi}H^{p,q,s}({\Bbb D})上的紧算子.

(7) 若 q+1=0, 则 C_{\varphi}H^{p,q,s}({\Bbb D}) 上的紧算子当且仅当 \| \varphi\| _{\infty}<1.

(8) 当 0<s<1 时, 若 C_{\varphi}H^{p,q,s}({\Bbb D}) 上的有界算子, 则对任意 t>0

\sup_{0\leq \rho<1, a, w\in {\Bbb D}}(1-\rho^{2})^{q}\int_{0}^{2\pi}\frac{(1-|w|^{2})^{t}(1-|\varphi_{a}(\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}}{|1-\overline{w}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{q+1+t}}\ {\rm d}\theta<\infty.
(3.3)

(9) 当 0<s<1q+s>0 时, 如果 p>1 取任意 \beta >(q+1)/p-1 或者 0<p\leq 1 取任意 \beta>q+\max\{s,p\}-1, 若

\sup_{0\leq\tau\leq 2\pi}\int_{0}^{2\pi}\frac{(1-|a|^{2})^{s}|1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s}\ {\rm d}\theta}{(1-|\varphi(a)|^{2})^{s}|1-r {\rm e}^{-{\rm i}\tau}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2+\beta}|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}}\lesssim \frac{1}{(1-r\rho)^{\beta+1}}
(3.4)

对所有 a\in {\Bbb D}0\leq r,\rho<1 成立, 则 C_{\varphi}H^{p,q,s}({\Bbb D}) 上的有界算子.

(10) 当 0<s<1q+s>0 时, 若(3.4)式成立, 则 C_{\varphi}H^{p,q,s}({\Bbb D}) 上的紧算子当且仅当(3.1)式成立.

为了下面的证明, 我们首先选取参数

\alpha>\max\left\{\frac{q+1}{p}-1, \ \frac{q+s}{p}-1, \ \frac{q+s+1}{p}-2\right\}.

(1) 若 \varphi 是一个自同构, 则存在酉变换 U 和对合自同构 \varphi_{a_{0}} 使得 \varphi=\varphi_{a_{0}}\circ U, 其中 a_{0}=\varphi(0). 因此, 我们仅需证明 \varphi 是酉变换或者对合自同构时结论成立.

\varphi 是一个酉变换时, 设 \varphi(z)=\lambda z (z\in {\Bbb D}), 其中 \lambda 是一个复常数满足 |\lambda|=1. 对任意 g\in H^{p,q,s}({\Bbb D}), 我们有

\begin{eqnarray*} \| C_{\varphi}g\| _{p,q,s}^{p}&=&\sup_{0\leq \rho<1}\sup_{a\in {\Bbb D}}(1-\rho^{2})^{q}\int_{0}^{2\pi}|g[\varphi(\rho {\rm e}^{{\rm i}\theta})]|^{p}(1-|\varphi_{a}(\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}\ \frac{{\rm d}\theta}{2\pi} \\ &=&\sup_{0\leq \rho<1}\sup_{ \lambda a\in {\Bbb D}}(1-|\lambda\rho|^{2})^{q}\int_{0}^{2\pi}|g(\lambda\rho {\rm e}^{{\rm i}\theta})|^{p} (1-|\varphi_{\lambda a}(\lambda\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}\ \frac{{\rm d}\theta}{2\pi}\\ &=&\| g\| _{p,q,s}^{p}. \end{eqnarray*}

这表明 C_{\varphi}H^{p,q,s}({\Bbb D}) 上有界且 \| \cdot\| _{p,q,s} 是酉不变的.

\varphi 是一个对合自同构时, 根据 \| \cdot\| _{p,q,s} 酉不变性可设 \varphi=\varphi_{a_{0}} 满足 a_{0}=\varphi(0)\geq 0. 对任意 0\leq\rho<1, 0\leq \theta\leq 2\pi, a\in {\Bbb D}, 根据变量替换 \xi=\varphi_{a_{0}}(\rho {\rm e}^{{\rm i}\theta}) 可得

\xi=c_{0}+r{\rm e}^{{\rm i}\tau}=\frac{a_{0}-\rho {\rm e}^{{\rm i}\theta}}{1-a_{0}\rho {\rm e}^{{\rm i}\theta}}, \ \ c_{0}=\frac{(1-\rho^{2})a_{0}}{1-\rho^{2}a_{0}^{2}}, \ \ r=\frac{\rho(1-a_{0}^{2})}{1-\rho^{2}a_{0}^{2}}, \ \ c_{0}+r=\frac{a_{0}+\rho}{1+\rho a_{0}}, 1-c_{0}a_{0}=\frac{r}{\rho}, \ \ {\rm d}\theta=\frac{\varphi'_{a_{0}}(c_{0}+r{\rm e}^{{\rm i}\tau})r{\rm e}^{{\rm i}\tau}\ {\rm d}\tau}{\varphi_{a_{0}}(c_{0}+r{\rm e}^{{\rm i}\tau})}=\frac{1-\rho^{2}a_{0}^{2}}{|1-\rho a_{0}{\rm e}^{{\rm i}\tau}|^{2}}\ {\rm d}\tau.
(3.5)

根据(3.5)式和 a=\varphi_{a_{0}}[\varphi_{a_{0}}(a)], 结合文献[9]中引理 1.3 可得

\begin{matrix} &\;& (1-\rho^{2})^{q}\int_{0}^{2\pi}|g[\varphi_{a_{0}}(\rho {\rm e}^{{\rm i}\theta})]|^{p}(1-|\varphi_{a}(\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}\ {\rm d}\theta \\ &\; =&(1-\rho^{2})^{q+s}(1-|a|^{2})^{s}\int_{0}^{2\pi}\frac{|g(c_{0}+r{\rm e}^{{\rm i}\tau})|^{p}(1-\rho^{2}a_{0}^{2})\ {\rm d}\tau}{|1-\rho a_{0}{\rm e}^{{\rm i}\tau}|^{2}|1-\overline{a}\varphi_{a_{0}}(c_{0}+r{\rm e}^{{\rm i}\tau})|^{2s}} \\ &\; =&\frac{(1-\rho^{2})^{q+s}(1-|a|^{2})^{s}(1-a_{0}^{2})^{2s}}{(1-\rho^{2}a_{0}^{2})^{2s-1}|1-a_{0}\overline{a}|^{2s}}\int_{0}^{2\pi}\frac{|g(c_{0}+r{\rm e}^{{\rm i}\tau})|^{p} \ {\rm d}\tau}{|1-\rho a_{0}{\rm e}^{{\rm i}\tau}|^{2-2s}|1-\overline{a}\varphi_{a_{0}}(c_{0}+r{\rm e}^{{\rm i}\tau})|^{2s}} \\ &\asymp&(1-\rho^{2})^{q+s}(1-|a|^{2})^{s}\int_{0}^{2\pi}\frac{|g(c_{0}+r{\rm e}^{{\rm i}\tau})|^{p}\ {\rm d}\tau}{|1-\overline{\varphi_{a_{0}}(a)}(c_{0}+r{\rm e}^{{\rm i}\tau})|^{2s}}. \end{matrix}
(3.6)

我们考虑函数

F(u)=\frac{g(u)}{(1-\overline{\varphi_{a_{0}}(a)}\ u)^{\frac{2s}{p}}} \ \ \ (u\in {\Bbb D}).

根据条件 \alpha>(q+1)/p-1 和引理 2.1, 2.2可得

\begin{equation} F(w)=\int_{{\Bbb D}}\frac{F(u)}{(1-w\overline{u})^{2+\alpha}}\ {\rm d}v_{\alpha}(u) \ \ (w\in {\Bbb D}). \end{equation}
(3.7)

(i) 情形 q+s>0.

p>1 时, 条件 \alpha> (q+s)/p-1q+s>0表明我们可以取 \max\{\alpha, q+s-1\}<\alpha_{1}<\min\{p(\alpha+1)-1, q+s+\alpha\}, 使得 (p\alpha-\alpha_{1})/(p-1)>-1, \ \alpha_{1}-\alpha>0, \ \alpha_{1}-q-s>-1, q+s-\alpha_{1}+\alpha>0. 由(3.7)式和 Hölder 不等式以及(3.5)式可得

\begin{matrix} |F(c_{0}+r{\rm e}^{{\rm i}\tau})|^{p}&\leq&\left(\int_{{\Bbb D}}\frac{|F(u)|\ {\rm d}v_{\alpha}(u)}{|1-(c_{0}+r{\rm e}^{{\rm i}\tau})\overline{u}|^{2+\alpha}}\right)^{p} \\ & \lesssim& \int_{{\Bbb D}}\frac{|F(u)|^{p}(1-|u|^{2})^{\alpha_{1}} {\rm d}v(u)}{|1- (c_{0}+r{\rm e}^{{\rm i}\tau})\overline{u}|^{2+\alpha}}\left(\int_{{\Bbb D}}\frac{(1-|u|^{2})^{\frac{p\alpha-\alpha_{1}}{p-1}}\ {\rm d}v(u)}{|1- (c_{0}+r{\rm e}^{{\rm i}\tau})\overline{u}|^{2+\alpha}}\right)^{p-1} \\ & \asymp&\frac{1}{(1-|c_{0}+r{\rm e}^{{\rm i}\tau}|^{2})^{\alpha_{1}-\alpha}}\int_{{\Bbb D}}\frac{|F(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\ {\rm d}v(u)}{|1- (c_{0}+r{\rm e}^{{\rm i}\tau})\overline{u}|^{2+\alpha}} \\ & \lesssim&\frac{1}{(1-\rho^{2})^{\alpha_{1}-\alpha}}\int_{{\Bbb D}}\frac{|F(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\ {\rm d}v(u)}{|1-(c_{0}+r{\rm e}^{{\rm i}\tau})\overline{u}|^{2+\alpha}}. \end{matrix}
(3.8)

c_{0}+r=(a_{0}+\rho)/(1+\rho a_{0})<1, 故 r|\overline{u}|<1-c_{0}|\overline{u}|\leq |1-c_{0}\overline{u}|. 因此,

\left|\frac{r\overline{u}}{1-c_{0}\overline{u}}\right|<1 \ \ \mbox{对任意 $u\in D$ 成立}.

由(3.6),(3.8)式, Fubini 定理, 引理 2.3, 文献[9,引理 1.8], \alpha_{1}-q-s>-1, q+s-\alpha_{1}+\alpha>0, 文献[引理 6], 文献[9,引理1.2], c_{0}+r=(a_{0}+\rho)/(1+\rho a_{0}), 我们可得

\begin{eqnarray*} &\;& (1-\rho^{2})^{q}\int_{0}^{2\pi}|g[\varphi_{a_{0}}(\rho {\rm e}^{{\rm i}\theta})]|^{p} (1-|\varphi_{a}(\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}\ {\rm d}\theta \\ &\;\lesssim & \int_{{\Bbb D}}|F(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\left\{\int_{0}^{2\pi}\frac{(1-\rho^{2})^{q+s+\alpha-\alpha_{1}}(1-|a|^{2})^{s}\ {\rm d}\tau}{|1-(c_{0}+r{\rm e}^{{\rm i}\tau})\overline{u}|^{2+\alpha}}\right\}{\rm d}v(u)\\ &\; =&\int_{{\Bbb D}}\frac{|F(u)|^{p}(1-|u|^{2})^{\alpha_{1}}}{|1-c_{0}\overline{u}|^{2+\alpha}}\left\{\int_{0}^{2\pi}\frac{(1-\rho^{2})^{q+s+\alpha-\alpha_{1}}(1-|a|^{2})^{s}\ {\rm d}\tau}{|1-\frac{r\overline{u}}{1-c_{0}\overline{u}}\ {\rm e}^{{\rm i}\tau}|^{2+\alpha}}\right\}{\rm d}v(u)\\ &\; \asymp &(1-\rho^{2})^{q+s+\alpha-\alpha_{1}}(1-|a|^{2})^{s}\int_{{\Bbb D}}\frac{|1-c_{0}u|^{-1}|g(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\ {\rm d}v(u)}{|1-\overline{\varphi_{a_{0}}(a)}\ u|^{2s}\{|1-c_{0}u|-r|u|\}^{\alpha+1}}\\ &\; \lesssim &(1-\rho^{2})^{q+s+\alpha-\alpha_{1}}(1-|a|^{2})^{s}\int_{{\Bbb D}}\frac{|g(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\ {\rm d}v(u)}{|1-\overline{\varphi_{a_{0}}(a)}\ u|^{2s}\{1-(c_{0}+r)|u|\}^{\alpha+1}} \\ &\; =&(1-\rho^{2})^{q+s+\alpha-\alpha_{1}}(1-|a|^{2})^{s}\int_{0}^{1}\frac{2t(1-t^{2})^{\alpha_{1}}}{\{1-(c_{0}+r)t\}^{\alpha+1}}\frac{(1-t^{2})^{-s-q}}{(1-|\varphi_{a_{0}}(a)|^{2})^{s}} \\ &\;& \times \left\{(1-t^{2})^{q}\int_{0}^{2\pi}|g(t{\rm e}^{{\rm i}\theta})|^{p}(1-|\varphi_{\varphi_{a_{0}}(a)}(t{\rm e}^{{\rm i}\theta})|^{2})^{s}\ \frac{{\rm d}\theta}{2\pi}\right\}{\rm d}t \\ &\; \lesssim & \frac{(1-\rho)^{q+s-\alpha_{1}+\alpha}(1-|a|^{2})^{s}}{(1-|\varphi_{a_{0}}(a)|^{2})^{s}}\| g\| ^{p}_{p,q,s}\int_{0}^{1}\frac{(1-t)^{\alpha_{1}-q-s}\ {\rm d}t}{\{1-(c_{0}+r)t\}^{\alpha+1}}\\ &\; \asymp &\frac{(1-\rho)^{q+s-\alpha_{1}+\alpha}}{\{1-(c_{0}+r)\}^{q+s-\alpha_{1}+\alpha}}\| g\| ^{p}_{p,q,s}\asymp\| g\| ^{p}_{p,q,s}. \end{eqnarray*}

0<p\leq 1 时, 设 \alpha=(2+\alpha')/p-2. 条件 \alpha>(q+s+1)/p-2 意味着 \alpha'>q+s-1. 由(3.7)式结合文献[9,引理 2.15] 可得

\begin{equation} |F(c_{0}+r{\rm e}^{{\rm i}\tau})|^{p}\leq \left(\int_{{\Bbb D}}\frac{|F(u)|\ {\rm d}v_{\alpha}(u)}{|1-(c_{0}+r{\rm e}^{{\rm i}\tau})\overline{u}|^{2+\alpha}}\right)^{p} \lesssim \int_{{\Bbb D}}\frac{|F(u)|^{p}\ (1-|u|^{2})^{\alpha'} {\rm d}v(u)}{|1-(c_{0}+r{\rm e}^{{\rm i}\tau})\overline{u}|^{2+\alpha'}}. \end{equation}
(3.9)

由(3.6)和(3.9)式, Fubini 定理, r|\overline{u}|/|1-c_{0}\overline{u}|<1, 引理 2.3, 文献[9,引理 1.8], \alpha'-q-s>-1, 文献[引理 6], q+s>0, c_{0}+r=(a_{0}+\rho)/(1+\rho a_{0}), 我们可得

\begin{eqnarray*} &\;& (1-\rho^{2})^{q}\int_{0}^{2\pi}|g[\varphi_{a_{0}}(\rho {\rm e}^{{\rm i}\theta})]|^{p} (1-|\varphi_{a}(\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}\ {\rm d}\theta \\ &\;\lesssim &\int_{{\Bbb D}}|F(u)|^{p}(1-|u|^{2})^{\alpha'}\left\{\int_{0}^{2\pi}\frac{(1-\rho^{2})^{q+s}(1-|a|^{2})^{s}\ {\rm d}\tau}{|1-(c_{0}+r{\rm e}^{{\rm i}\tau})\overline{u}|^{2+\alpha'}}\right\}{\rm d}v(u) \\ &\; \lesssim &(1-\rho^{2})^{q+s}(1-|a|^{2})^{s}\int_{{\Bbb D}}\frac{|g(u)|^{p}(1-|u|^{2})^{\alpha'}\ {\rm d}v(u)}{|1-\overline{\varphi_{a_{0}}(a)}\ u|^{2s}\{1-(c_{0}+r)|u|\}^{\alpha'+1}}\\ &\; \lesssim &\frac{(1-\rho)^{q+s}(1-|a|^{2})^{s}}{(1-|\varphi_{a_{0}}(a)|^{2})^{s}}\| g\| ^{p}_{p,q,s}\int_{0}^{1}\frac{(1-t)^{\alpha'-q-s}\ {\rm d}t}{\{1-(c_{0}+r)t\}^{\alpha'+1}}\asymp\| g\| ^{p}_{p,q,s}. \end{eqnarray*}

(ii) 情形 q+s=0.

在这种情形下, H^{p,q,s}({\Bbb D})\subseteq H^{p}({\Bbb D}), 因而 g({\rm e}^{{\rm i}\tau}) [2\pi] 上几乎处处有定义. 根据解析函数积分平均的递增性和文献[9,引理1.3]结合(3.5)式, 我们可得

\begin{eqnarray*} (1-|a|^{2})^{s}\int_{0}^{2\pi}\left|\frac{g[\varphi_{a_{0}}(\rho {\rm e}^{{\rm i}\theta})]}{(1-\overline{a}\rho {\rm e}^{{\rm i}\theta})^{\frac{2s}{p}}}\right|^{p} {\rm d}\theta & \leq&(1-|a|^{2})^{s}\int_{0}^{2\pi}\left|\frac{g[\varphi_{a_{0}}( {\rm e}^{{\rm i}\theta})]}{(1-\overline{a} {\rm e}^{{\rm i}\theta})^{\frac{2s}{p}}}\right|^{p} {\rm d}\theta\\ &\; =&(1-|a|^{2})^{s}\int_{0}^{2\pi}\left|\frac{g({\rm e}^{{\rm i}\tau})}{\{1-\overline{a}\varphi_{a_{0}}({\rm e}^{{\rm i}\tau})\}^{\frac{2s}{p}}}\right|^{p} \frac{1-a_{0}^{2}}{|1-a_{0}{\rm e}^{{\rm i}\tau}|^{2}}\ {\rm d}\tau\\ &\; =&(1-|a|^{2})^{s}\int_{0}^{2\pi}\frac{|g({\rm e}^{{\rm i}\tau})|^{p}|1-a_{0}{\rm e}^{{\rm i}\tau}|^{2s-2}(1-a_{0}^{2})}{|1-a_{0}\overline{a}|^{2s}|1-\overline{\varphi_{a_{0}}(a)}{\rm e}^{{\rm i}\tau}|^{2s}}\ {\rm d}\tau\\ &\; \asymp &\int_{0}^{2\pi}\frac{|g({\rm e}^{{\rm i}\tau})|^{p}\ (1-|\varphi_{a_{0}}(a)|^{2})^{s}}{|1-\overline{\varphi_{a_{0}}(a)}{\rm e}^{{\rm i}\tau}|^{2s}}\ \frac{{\rm d}\tau}{2\pi}\leq\| g\| _{p,q,s}^{p}. \end{eqnarray*}

总之, 对所有 q+s\geq 0, 我们都有 \| C_{\varphi}g\| _{p,q,s}\lesssim \| g\| _{p,q,s}.

(2) 根据文献[5,命题3.3], 当 s\geq 1> -q 时, H^{p,q,s}({\Bbb D})=H^{\infty}_{\frac{q+1}{p}}({\Bbb D});当 s\geq 1=-q 时, H^{p,q,s}({\Bbb D})=H^{\infty}({\Bbb D}). 因此, 当 s\geq 1\geq -q 时, C_{\varphi}H^{p,q,s}({\Bbb D}) 上总是有界的. 我们仅仅需要证明情形 s=0\leq q 时的结果. 实际上, \varphi=\varphi_{a_{0}}\circ\psi, 其中 a_{0}=\varphi(0)\psi: {\Bbb D}\rightarrow {\Bbb D} 是一个解析映射且满足 \psi(0)=0. 对任意 g\in H^{p,q,s}({\Bbb D})0\leq\rho<1, 根据引理 2.4 可得

(1-\rho^{2})^{q}\int_{0}^{2\pi}|g[\varphi(\rho {\rm e}^{{\rm i}\theta})]|^{p}\ {\rm d}\theta \leq (1-\rho^{2})^{q}\int_{0}^{2\pi}|g[\varphi_{a_{0}}(\rho {\rm e}^{{\rm i}\theta})]|^{p} {\rm d}\theta.

余下的证明和(1)中情形 s=0 时相同.

(3) 当 \| \varphi\| _{\infty}=\sup \{ |\varphi(z)|: z\in D \}<1 时,(3.1)式是显然的. 当 \| \varphi\| _{\infty}=1 时, 设 \{w^{j}\}\subset {\Bbb D} 是任一使得 |\varphi(w^{j})|\rightarrow 1 (j\rightarrow\infty) 的序列. 我们取

g_{j}(w)=\frac{(1-|\varphi(w^{j})|^{2})^{\frac{|q|}{p}+1}}{(1- w\overline{\varphi(w^{j})})^{\frac{q+1+|q|}{p}+1}} \ \ \ (w\in {\Bbb D}).

\{g_{j}\}{\Bbb D} 的任一紧子集上一致趋于0. 根据引理 2.5, 分三种情况 0\leq 2s<1, 2s=1, 2s>1, 容易证明\sup \{\| g_{j}\| _{p,q,s}: j=1,2,\cdots \}\lesssim 1 (可参见文献[5]). 因此, 由引理2.1可得

\begin{equation} \left(\frac{1-|w^{j }|^{2}}{1-|\varphi(w^{j})|^{2}}\right)^{\frac{q+1}{p}}=(1-|w^{j}|^{2})^{\frac{q+1}{p}}|C_{\varphi}g_{j}(w^{j})|\lesssim \| C_{\varphi}g_{j}\| _{p,q,s}\rightarrow 0 \ \ (j\rightarrow\infty). \end{equation}
(3.10)

这表明(3.1)式成立.

(4) 必要性在结论 (3)中已经证明. 下面我们证充分性.

设序列 \{h_{k}\}{\Bbb D} 的任一紧子集上一致趋于0, 且对所有 k\in \{1,2,\cdots\}满足 \| h_{k}\| _{p,q,s}\leq 1.s\geq 1>-q 时, H^{p,q,s}({\Bbb D})=H^{\infty}_{\frac{q+1}{p}}({\Bbb D}).(3.1) 式成立, 容易证明 \| C_{\varphi}h_{k}\| _{p,q,s}\rightarrow0 \ (k\rightarrow\infty).s=0<q 时, 对任意 k\in \{1,2,\cdots\}\rho\in (1/2,1), 由(3.7)式, 我们可以取

T_{\rho}h_{k}(w)=\int_{{\Bbb D}}H_{\rho}(w,u)h_{k}(u)\ {\rm d}v_{\alpha}(u),

其中

H_{\rho}(w,u)=\frac{\chi_{\rho}(w)}{ |1-\varphi(w)\overline{u}|^{2+\alpha}} \ \ (w,\ u \in {\Bbb D}),

\chi_{\rho} 表示集合 \{z: \rho<|z|<1\} 的特征函数. 设 a_{0}=\varphi(0)

M_{\rho}=\sup_{\rho<|z|<1}\frac{1-|z|^{2}}{1-|\varphi(z)|^{2}}.

p>1 时, 条件 \alpha> q/p-1q>0 意味着我们可以取 \max\{\alpha, q-1\}<\alpha_{1}<\min\{p(\alpha+1)-1, q+\alpha\} 使得 \left(\alpha-\frac{\alpha_{1}}{p}\right)\frac{p}{p-1}>-1, \ \alpha_{1}-\alpha>0, \ \alpha_{1}-q>-1, \ q-\alpha_{1}+\alpha>0.|w|>\rho 时, 根据 Hölder 不等式和引理2.3可得

\begin{matrix} \{T_{\rho}(|h_{k}|)(w)\}^{p}&\lesssim& \frac{\chi_{\rho}(w)}{(1-|\varphi(w)|^{2})^{\alpha_{1}-\alpha}}\int_{{\Bbb D}}\frac{|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\ {\rm d}v(u)}{|1-\varphi(w)\overline{u}|^{2+\alpha}} \\ &\leq &\frac{M_{\rho}^{\alpha_{1}-\alpha}}{(1-|w|^{2})^{\alpha_{1}-\alpha}}\int_{{\Bbb D}}\frac{|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\ {\rm d}v(u)}{|1-\varphi(w)\overline{u}|^{2+\alpha}}. \end{matrix}
(3.11)

如果 1/2<r<1u\in {\Bbb D}, 我们有

\begin{matrix} 1-r^{2}|\varphi_{a_{0}}(u)|^{2} & = & 1-r^{2}+\frac{r^{2}(1-|a_{0}|^{2})(1-|u|^{2})}{|1-\overline{a_{0}}u|^{2}} \\ & \geq& 1-r^{2}+\frac{1-|a_{0}|}{4(1+|a_{0}|)}(1-|u|^{2}) \\ &\geq& \frac{1-|a_{0}|}{4(1+|a_{0}|)}(2-r-|u|) \\ &\geq& \frac{1-|a_{0}|}{4(1+|a_{0}|)}(1-r|u|). \end{matrix}
(3.12)

如果 0\leq r\leq 1/2u\in {\Bbb D}, 我们有

\begin{equation} 1-r^{2}|\varphi_{a_{0}}(u)|^{2}\geq \frac{3}{4}\geq \frac{3(2-r-|u|)}{8}\geq \frac{3(1-r|u|)}{8}. \end{equation}
(3.13)

\varphi=\varphi_{a_{0}}\circ\psi 满足 \psi(0)=0.\rho<r<1时, 根据 Fubini 定理, 引理 2.4, 文献[9,引理1.3和引理1.8],(3.11)-(3.13)式, \alpha_{1}-q>-1, q-\alpha_{1}+\alpha>0, 文献[引理6], 可得

\begin{matrix} &\;& (1-r^{2})^{q}\int_{0}^{2\pi}\{T_{\rho}(|h_{k}|)(r{\rm e}^{{\rm i}\theta})\}^{p}\ {\rm d}\theta \\ &\lesssim& M_{\rho}^{\alpha_{1}-\alpha}(1-r^{2})^{q+\alpha-\alpha_{1}} \int_{{\Bbb D}}|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\left\{\int_{0}^{2\pi}\frac{ {\rm d}\theta}{|1-\varphi_{a_{0}}[\psi(r{\rm e}^{{\rm i}\theta})]\overline{u}|^{2+\alpha}}\right\}{\rm d}v(u) \\ &\; \leq & \int_{{\Bbb D}}|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\left\{\int_{0}^{2\pi}\frac{ M_{\rho}^{\alpha_{1}-\alpha}(1-r^{2})^{q+\alpha-\alpha_{1}}\ {\rm d}\theta}{|1-\varphi_{a_{0}}(r{\rm e}^{{\rm i}\theta})\overline{u}|^{2+\alpha}}\right\}{\rm d}v(u) \\ &\; \asymp & \int_{{\Bbb D}}|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\left\{\int_{0}^{2\pi}\frac{ M_{\rho}^{\alpha_{1}-\alpha}(1-r^{2})^{q+\alpha-\alpha_{1}}\ {\rm d}\theta}{|1- r{\rm e}^{{\rm i}\theta}\overline{\varphi_{a_{0}}(u)}|^{2+\alpha}}\right\}{\rm d}v(u) \\ &\; \asymp & M_{\rho}^{\alpha_{1}-\alpha}(1-r^{2})^{q+\alpha-\alpha_{1}}\int_{{\Bbb D}}\frac{|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\ {\rm d}v(u)}{(1-r^{2}|\varphi_{a_{0}}(u)|^{2})^{1+\alpha}} \\ &\; \lesssim & M_{\rho}^{\alpha_{1}-\alpha}(1-r^{2})^{q+\alpha-\alpha_{1}}\int_{{\Bbb D}}\frac{|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha_{1}}\ {\rm d}v(u)}{(1-r|u|)^{1+\alpha}} \\ &\lesssim& M_{\rho}^{\alpha_{1}-\alpha}(1-r)^{q+\alpha-\alpha_{1}}\| h_{k}\| _{p,q,s}^{p}\int_{0}^{1}\frac{(1-t)^{\alpha_{1}-q}\ {\rm d}t}{(1-rt)^{1+\alpha}} \lesssim M_{\rho}^{\alpha_{1}-\alpha}. \end{matrix}
(3.14)

根据(3.7)(情形 s=0) 和(3.14)式, 有

\begin{eqnarray*} &\;& \sup_{0\leq r<1}(1-r^{2})^{q}\int_{0}^{2\pi}|h_{k}[\varphi(r {\rm e}^{{\rm i}\theta})]|^{p}\ {\rm d}\theta\\ &\lesssim& \sup_{0\leq r\leq \rho}(1-r^{2})^{q}\int_{0}^{2\pi}|h_{k}[\varphi(r {\rm e}^{{\rm i}\theta})]|^{p}\ {\rm d}\theta +\sup_{\rho< r<1}(1-r^{2})^{q}\int_{0}^{2\pi}\{T_{\rho}(|h_{k}|)(r{\rm e}^{{\rm i}\theta})\}^{p}\ {\rm d}\theta\\ & \lesssim &\sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p}+M_{\rho}^{\alpha_{1}-\alpha}\rightarrow M_{\rho}^{\alpha_{1}-\alpha} \ \ (k\rightarrow\infty). \end{eqnarray*}

因而当(3.1)式成立时我们有 \| C_{\varphi}h_{k}\| _{p,q,s}\rightarrow0 \ (k\rightarrow\infty). 这表明 C_{\varphi}H^{p,q,s}({\Bbb D})上的紧算子.

0<p\leq 1时, 设 \alpha=(2+\alpha')/p-2, 这意味着 \alpha'>q-1. 我们选取 0<\varepsilon<\min\{q,1+\alpha'\}. 由(3.7)式, 文献[9,引理2.15], Fubini 定理, 文献[9,引理 1.8], 引理 2.4, 文献[9,引理 1.3], 文献[引理 6], 我们可得

\begin{matrix} &\;& \sup_{0\leq t<1}(1-t^{2})^{q}\int_{0}^{2\pi}|h_{k}[\varphi(t {\rm e}^{{\rm i}\theta})]|^{p}\ {\rm d}\theta \\ &\lesssim& \sup_{0\leq t\leq \rho}(1-t^{2})^{q}\int_{0}^{2\pi}|h_{k}[\varphi(t {\rm e}^{{\rm i}\theta})]|^{p}\ {\rm d}\theta \\ &&+\sup_{\rho< t<1} \int_{{\Bbb D}}|h_{k}(u)|^{p}\left\{\int_{0}^{2\pi}\frac{ (1-t^{2})^{q}(1-|u|^{2})^{\alpha'} \ {\rm d}\theta}{|1- \varphi(t{\rm e}^{{\rm i}\theta})\overline{u}|^{2+\alpha'}}\right\}{\rm d}v(u) \\ &\lesssim& \sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p} + M_{\rho}^{\varepsilon}\sup_{\rho< t<1} \int_{{\Bbb D}}|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha'}\left\{\int_{0}^{2\pi}\frac{ (1-t^{2})^{q-\varepsilon} \ {\rm d}\theta}{|1- u\overline{\varphi(t{\rm e}^{{\rm i}\theta})}|^{2+\alpha'-\varepsilon}}\right\}{\rm d}v(u) \\ & \leq&\sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p}+\sup_{\rho< t<1} \int_{{\Bbb D}}|h_{k}(u)|^{p}\left\{\int_{0}^{2\pi}\frac{M_{\rho}^{\varepsilon}(1-|u|^{2})^{\alpha'} (1-t^{2})^{q-\varepsilon} {\rm d}\theta}{|1- u\overline{\varphi_{a_{0}}(t{\rm e}^{{\rm i}\theta})}|^{2+\alpha'-\varepsilon}}\right\}{\rm d}v(u) \\ & \asymp&\sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p}+\sup_{\rho< t<1} \int_{{\Bbb D}}|h_{k}(u)|^{p}\left\{\int_{0}^{2\pi}\frac{M_{\rho}^{\varepsilon}(1-|u|^{2})^{\alpha'} (1-t^{2})^{q-\varepsilon} {\rm d}\theta}{|1- \overline{\varphi_{a_{0}}(u)}t{\rm e}^{{\rm i}\theta}|^{2+\alpha'-\varepsilon}}\right\}{\rm d}v(u) \\ & \asymp&\sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p}+\sup_{\rho< t<1} \int_{{\Bbb D}}|h_{k}(u)|^{p}\left\{\frac{M_{\rho}^{\varepsilon}(1-|u|^{2})^{\alpha'} (1-t^{2})^{q-\varepsilon}}{(1-t^{2}|\varphi_{a_{0}}(u)|^{2})^{1+\alpha'-\varepsilon}}\right\}{\rm d}v(u) \\ & \lesssim &\sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p}+M_{\rho}^{\varepsilon}\sup_{\rho< t<1} (1-t^{2})^{q-\varepsilon}\int_{{\Bbb D}}\frac{|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha'}\ {\rm d}v(u)}{(1-t|u|)^{1+\alpha'-\varepsilon}} \\ & \lesssim& \sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p}+M_{\rho}^{\varepsilon}\sup_{\rho< t<1} (1-t)^{q-\varepsilon}\| h_{k}\| _{p,q,s}^{p}\int_{0}^{1}\frac{(1-\varrho)^{\alpha'-q}\ {\rm d}\varrho}{(1-t\varrho)^{1+\alpha'-\varepsilon}} \\ &\lesssim &\sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p}+M_{\rho }^{\varepsilon}\rightarrow M_{\rho}^{\varepsilon} \ \ (k\rightarrow\infty). \end{matrix}
(3.15)

根据(3.1)和(3.15)式可得 C_{\varphi}H^{p,q,s}({\Bbb D})上的紧算子.

(5) 该结果来自文献[7,定理 3.20].

(6) 如果 \| \varphi\| _{\infty}<1, 则任意序列\{h_{k}\}满足在{\Bbb D}的任一紧子集上一致趋于0且 \| h_{k}\| _{p,q,s}\leq 1 对所有 k 成立时有

\begin{eqnarray*} &&\sup_{0\leq \rho<1}\sup_{a\in {\Bbb D}}(1-\rho^{2})^{q}\int_{0}^{2\pi}|h_{k}[\varphi(\rho {\rm e}^{{\rm i}\theta})]|^{p}(1-|\varphi_{a}(\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}\ {\rm d}\theta \\ &\leq &\max_{|w|\leq \| \varphi\| _{\infty}}|h_{k}(w)|^{p}\sup_{0\leq \rho<1}\sup_{a\in {\Bbb D}}\int_{0}^{2\pi}\frac{(1-\rho^{2})^{q+s}(1-|a|^{2})^{s}\ {\rm d}\theta}{|1-\rho\overline{a} {\rm e}^{{\rm i}\theta}|^{2s}} \\ &\lesssim& \max_{|w|\leq \| \varphi\| _{\infty}}|h_{k}(w)|^{p} \ \rightarrow 0 \ \ (k\rightarrow\infty) \ \Rightarrow \ \mbox{$C_{\varphi}$ 是 $H^{p,q,s}({\Bbb D})$上的紧算子.} \end{eqnarray*}

(7) 当 q+1=0\| \varphi\| _{\infty}=1时, 假如 C_{\varphi}H^{p,q,s}({\Bbb D})上的紧算子, 我们可导出与(3.10)式矛盾.

(8) 对任意 w\in {\Bbb D}t>0, 设

f_{w}(z)=\frac{(1-|w|^{2})^{\frac{t}{p}}}{(1-z\overline{w})^{\frac{q+1+t}{p}}} \ \ (z\in {\Bbb D}).

根据引理 2.5(1)-(6), 容易证明 \sup \{\| f_{w}\| _{p,q,s}: w\in {\Bbb D}\}\lesssim 1. 根据C_{\varphi}H^{p,q,s}({\Bbb D})上的有界性可得(3.3)式成立.

(9) 对任意 g\in H^{p,q,s}({\Bbb D})a\in {\Bbb D}, 取

G_{a,g}(w)=\frac{g(w)}{(1-\overline{\varphi(a)}w)^{\frac{2s}{p}}} \ \ (w\in {\Bbb D}).

根据引理 2.1, 2.2 可得

G_{a,g}(w)=\int_{{\Bbb D}}\frac{G_{a,g}(u)\ {\rm d}v_{\alpha}(u)}{(1-w\overline{u})^{2+\alpha}} \ \ (w\in {\Bbb D}).

因此,

|G_{a,g}[\varphi(z)]|\leq \int_{{\Bbb D}}\frac{|G_{a,g}(u)|\ {\rm d}v_{\alpha}(u)}{|1-\varphi(z) \overline{u}|^{2+\alpha}} \ \ (z\in {\Bbb D}).
(3.16)

对任意 0\leq \rho<1, 若 p>1\max\{0, -q\}<s<1, 由条件 \alpha>(q+1)/p-1 可选择

\max\{\alpha, \ q+s-1\}<\alpha_{1}<\min\{p(\alpha+1)-1, \ q+s+\alpha\}.

当(3.4)式成立时, 根据(3.16)式, Hölder 不等式,

(1-\rho^{2})/\{1-|\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2}\}\leq \{1+|\varphi(0)|\}/\{1-|\varphi(0)|\},

Fubini 定理, 文献[9,引理 1.8],(3.4)式, 文献[引理 6], 我们可得

\begin{eqnarray*} &\;& (1-\rho^{2})^{q}\int_{0}^{2\pi}|g[\varphi(\rho {\rm e}^{{\rm i}\theta})]|^{p}(1-|\varphi_{a}(\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}\ {\rm d}\theta\\ &\; =&(1-\rho^{2})^{q+s}(1-|a|^{2})^{s}\int_{0}^{2\pi}|G_{a,g}[\varphi(\rho {\rm e}^{{\rm i}\theta})]|^{p}\frac{|1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s}}{|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}}\ {\rm d}\theta\\ &\;\lesssim & (1-\rho^{2})^{q+s}(1-|a|^{2})^{s}\int_{0}^{2\pi}\left\{\int_{{\Bbb D}}\frac{|G_{a,g}(u)|\ {\rm d}v_{\alpha}(u)}{|1-\varphi(\rho {\rm e}^{{\rm i}\theta}) \overline{u}|^{2+\alpha}}\right\}^{p}\frac{|1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s}}{|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}}\ {\rm d}\theta \\ &\; \lesssim & \int_{0}^{2\pi}\int_{{\Bbb D}}\frac{(1-\rho^{2})^{q+s}(1-|a|^{2})^{s}|g(u)|^{p}|1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s} (1-|u|^{2})^{\alpha_{1}}\ {\rm d}v(u){\rm d}\theta}{(1-|\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2})^{\alpha_{1}-\alpha}|1-\varphi(\rho {\rm e}^{{\rm i}\theta}) \overline{u}|^{2+\alpha}|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}|1-\overline{\varphi(a)}u|^{2s}} \\ &\; \lesssim & \int_{0}^{2\pi}\int_{{\Bbb D}}\frac{(1-\rho^{2})^{q+s+\alpha-\alpha_{1}}|g(u)|^{p}|1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s} (1-|u|^{2})^{\alpha_{1}}}{(1-|a|^{2})^{-s}|1-\varphi(\rho {\rm e}^{{\rm i}\theta}) \overline{u}|^{2+\alpha}|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}|1-\overline{\varphi(a)}u|^{2s}}\ {\rm d}v(u){\rm d}\theta \\ &\; =&\int_{{\Bbb D}}\frac{|g(u)|^{p}(1-|u|^{2})^{\alpha_{1}}}{(1-|a|^{2})^{-s}|1-\overline{\varphi(a)}u|^{2s}}\int_{0}^{2\pi}\frac{(1-\rho^{2})^{q+s+\alpha-\alpha_{1}} |1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s}\ {\rm d}\theta {\rm d}v(u)}{|1-\varphi(\rho {\rm e}^{{\rm i}\theta}) \overline{u}|^{2+\alpha}|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}}\\ &\; \lesssim & \int_{0}^{1}(1-r^{2})^{\alpha_{1}-q-s}\int_{0}^{2\pi}(1-r^{2})^{q}|g(r {\rm e}^{{\rm i}\tau})|^{p}(1-|\varphi_{\varphi(a)}(r {\rm e}^{{\rm i}\tau})|^{2})^{s}\\ &\;& \times \left\{\frac{(1-|a|^{2})^{s}}{(1-|\varphi(a)|^{2})^{s}}\int_{0}^{2\pi}\frac{(1-\rho^{2})^{q+s+\alpha-\alpha_{1}}|1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s}\ {\rm d}\theta}{|1-r {\rm e}^{-{\rm i}\tau}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2+\alpha}|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}}\right\} {\rm d}\tau {\rm d}r\\ &\; \lesssim &(1-\rho)^{q+s+\alpha-\alpha_{1}}\| g\| _{p,q,s}^{p}\int_{0}^{1}\frac{(1-r)^{\alpha_{1}-q-s}}{(1-r\rho)^{\alpha+1}}\ {\rm d}r \lesssim \| g\| _{p,q,s}^{p}. \end{eqnarray*}

这意味着 C_{\varphi}H^{p,q,s}({\Bbb D})上的有界算子.

0<p\leq 1\max\{0, -q\}<s<1 时, 设 \alpha=(\alpha'+2)/p-2.\alpha>\max\{(q+1)/p-1,(q+s+1)/p-2\} 知, \alpha'>q+\max\{s,p\}-1. 若(3.4)式成立, 由(3.16)式, 文献[9,引理 2.15], Fubini 定理, 文献[9,引理 1.8],(3.4)式, 文献[引理 6], 有

\begin{eqnarray*} &\;& (1-\rho^{2})^{q}\int_{0}^{2\pi}|g[\varphi(\rho {\rm e}^{{\rm i}\theta})]|^{p}(1-|\varphi_{a}(\rho {\rm e}^{{\rm i}\theta})|^{2})^{s}\ {\rm d}\theta \\ &\; \lesssim &\int_{0}^{2\pi}\int_{{\Bbb D}}\frac{(1-\rho^{2})^{q+s}(1-|a|^{2})^{s}|g(u)|^{p}|1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s}(1-|u|^{2})^{\alpha'}}{|1-\varphi(\rho {\rm e}^{{\rm i}\theta}) \overline{u}|^{2+\alpha'}|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}|1-\overline{\varphi(a)}u|^{2s}}\ {\rm d}\theta {\rm d}v(u) \\ &\; =&\int_{{\Bbb D}}\frac{(1-|a|^{2})^{s}|g(u)|^{p}(1-|u|^{2})^{\alpha'}}{|1-\overline{\varphi(a)}u|^{2s}}\int_{0}^{2\pi}\frac{(1-\rho^{2})^{q+s} |1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s}\ {\rm d}\theta {\rm d}v(u)}{|1-\varphi(\rho {\rm e}^{{\rm i}\theta}) \overline{u}|^{2+\alpha'}|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}}\\ &\; \lesssim &\int_{0}^{1}(1-r^{2})^{\alpha'-q-s}\int_{0}^{2\pi}(1-r^{2})^{q}|g(r {\rm e}^{{\rm i}\tau})|^{p}(1-|\varphi_{\varphi(a)}(r {\rm e}^{{\rm i}\tau})|^{2})^{s}\\ &\;& \times \left\{\int_{0}^{2\pi}\frac{(1-|a|^{2})^{s}(1-\rho^{2})^{q+s}|1-\overline{\varphi(a)}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2s}\ {\rm d}\theta}{(1-|\varphi(a)|^{2})^{s}|1-r {\rm e}^{-{\rm i}\tau}\varphi(\rho {\rm e}^{{\rm i}\theta})|^{2+\alpha'}|1-\overline{a}\rho {\rm e}^{{\rm i}\theta}|^{2s}}\right\}{\rm d}\tau {\rm d}r \\ &\; \lesssim &(1-\rho)^{q+s}\| g\| _{p,q,s}^{p}\int_{0}^{1}\frac{(1-r)^{\alpha'-q-s}}{(1-r\rho)^{\alpha'+1}}\ {\rm d}r \lesssim \| g\| _{p,q,s}^{p}. \end{eqnarray*}

这表明 C_{\varphi}H^{p,q,s}({\Bbb D}) 上的有界算子.

(10) 设 \{h_{k}\} 是任一在 {\Bbb D} 的任一紧子集上一致趋于0 且满足 \| h_{k}\| _{p,q,s}\leq 1 对所有 k\in \{1,2,\cdots\} 成立的序列. 设 1/2<\rho<1.p>1 时, 类似(3.14)式的证明, 根据(3.16)和(3.4)式可得

\begin{eqnarray*} &\;& \sup_{0\leq r<1}(1-r^{2})^{q}\int_{0}^{2\pi}|h_{k}[\varphi(r{\rm e}^{{\rm i}\theta})]|^{p}(1-|\varphi_{a}(r{\rm e}^{{\rm i}\theta})|^{2})^{s}\ {\rm d}\theta\\ &\lesssim& \max_{|u|\leq \rho}|h_{k}[\varphi(u)]|^{p} +\sup_{\rho<r<1}(1-r^{2})^{q}\\ &&\times \int_{0}^{2\pi}(1-|\varphi_{a}(r{\rm e}^{{\rm i}\theta})|^{2})^{s}|G_{a,h_{k}}[\varphi(r{\rm e}^{{\rm i}\theta})]| ^{p}|1-\overline{\varphi(a)}\varphi(r{\rm e}^{{\rm i}\theta})|^{2s}\ {\rm d}\theta\\ & \lesssim& \max_{|u|\leq \rho}|h_{k}[\varphi(u)]|^{p}+M_{\rho}^{\alpha_{1}-\alpha}\sup_{\rho<r<1}(1-r^{2}) ^{q+s+\alpha-\alpha_{1}}(1-|a|^{2})^{s} \\ &\;& \times \int_{{\Bbb D}}\frac{|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha_{1}}}{|1-\varphi(a)\overline{u}|^{2s}} \left\{\int_{0}^{2\pi}\frac{|1-\overline{\varphi(a)}\varphi(r{\rm e}^{{\rm i}\theta})|^{2s} \ {\rm d}\theta}{|1-\varphi(r{\rm e}^{{\rm i}\theta})\overline{u}|^{2+\alpha}|1-r\overline{a}{\rm e}^{{\rm i}\theta}|^{2s}}\right\}{\rm d}v(u) \\ & \lesssim &\max_{|u|\leq \rho}|h_{k}[\varphi(u)]|^{p}+M_{\rho}^{\alpha_{1}-\alpha}\sup_{\rho<r<1}(1-r^{2})^{q+s+\alpha-\alpha_{1}}\\ \\ &\;& \times \int_{0}^{1}\frac{(1-t)^{\alpha_{1}-q-s}}{(1-rt)^{\alpha+1}}\left\{\int_{0}^{2\pi}(1-t^{2})^{q}|h_{k}(t{\rm e}^{{\rm i}\tau})|^{p}(1-|\varphi_{\varphi(a)}(t{\rm e}^{{\rm i}\tau})|^{2})^{s}\ {\rm d}\tau\right\}{\rm d}t \\ & \lesssim &\max_{|u|\leq \rho}|h_{k}[\varphi(u)]|^{p}+M_{\rho}^{\alpha_{1}-\alpha}\rightarrow M_{\rho}^{\alpha_{1}-\alpha} \ \ ( k\rightarrow\infty). \end{eqnarray*}

0<p\leq 1 时, 我们选取 0<\varepsilon<\min\{q+s, 1+\alpha'-q-\max\{s,p\}\}. 类似(3.15)式的证明, 根据(3.16)和(3.4)式可得

\begin{eqnarray*} &\;& \sup_{0\leq r<1,a\in D}(1-r^{2})^{q}\int_{0}^{2\pi}|h_{k}[\varphi(r{\rm e}^{{\rm i}\theta})]|^{p}(1-|\varphi_{a}(r{\rm e}^{{\rm i}\theta})|^{2})^{s}\ {\rm d}\theta\\ &\; \lesssim &\sup_{0\leq r\leq \rho,a\in D}(1-r^{2})^{q}\int_{0}^{2\pi}|h_{k}[\varphi(r {\rm e}^{{\rm i}\theta})]|^{p}(1-|\varphi_{a}(r{\rm e}^{{\rm i}\theta})|^{2})^{s}\ {\rm d}\theta+(1-|a|^{2})^{s}\\ &\;& \times\sup_{\rho< r<1,a\in D} \int_{{\Bbb D}}\frac{|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha'}}{|1-\overline{\varphi(a)}u|^{2s}}\int_{0}^{2\pi}\frac{ (1-r^{2})^{q+s}|1-\overline{\varphi(a)}\varphi(r{\rm e}^{{\rm i}\theta})|^{2s} \ {\rm d}\theta}{|1- u\overline{\varphi(r{\rm e}^{{\rm i}\theta})}|^{2+\alpha'}|1-r\overline{a}{\rm e}^{{\rm i}\theta}|^{2s}}\ {\rm d}v(u) \\ &\;\lesssim &\sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p}+\sup_{\rho<r<1,a\in D}M_{\rho}^{\varepsilon}(1-r^{2})^{q+s-\varepsilon}(1-|a|^{2})^{s}\\ &\;& \times \ \int_{{\Bbb D}}\frac{|h_{k}(u)|^{p}(1-|u|^{2})^{\alpha'}}{|1-\overline{\varphi(a)}u|^{2s}}\left\{\int_{0}^{2\pi}\frac{ |1-\overline{\varphi(a)}\varphi(r{\rm e}^{{\rm i}\theta})|^{2s} \ {\rm d}\theta}{|1- u\overline{\varphi(r{\rm e}^{{\rm i}\theta})}|^{2+\alpha'-\varepsilon}|1-r\overline{a}{\rm e}^{{\rm i}\theta}|^{2s}}\right\}{\rm d}v(u) \\ &\;\lesssim &\sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p} +M_{\rho}^{\varepsilon}\sup_{\rho<r<1}(1-r)^{q+s-\varepsilon}\| h_{k}\| _{p,q,s}^{p} \int_{0}^{1}\frac{(1-t)^{\alpha'-q-s}}{(1-rt)^{1+\alpha'-\varepsilon}} \ {\rm d}t \\ &\;\lesssim &\sup_{|w|\leq \rho}|h_{k}[\varphi(w)]|^{p}+M_{\rho}^{\varepsilon}\rightarrow M_{\rho}^{\varepsilon} \ \ (k\rightarrow\infty). \end{eqnarray*}

根据(3.1)式可得 C_{\varphi}H^{p,q,s}({\Bbb D}) 上的紧算子.

本定理证完.

根据文献[5,命题3.3]可知, 如果 0<s<1, 则 H^{\frac{p}{q+1}}({\Bbb D})\subsetneq H^{p,q,s}({\Bbb D}). 进一步, 我们有下列结果.

定理 3.20<s<1 以及 \varphi: \ {\Bbb D}\rightarrow {\Bbb D} 是一个解析映射.

(1) C_{\varphi} 总是 H^{\frac{p}{q+1}}({\Bbb D})H^{p,q,s}({\Bbb D}) 的有界算子.

(2) 若 C_{\varphi}H^{\frac{p}{q+1}}({\Bbb D})H^{p,q,s}({\Bbb D}) 的紧算子, 则(3.1)式成立.

(3) 若(3.2)式成立, 则 C_{\varphi}H^{\frac{p}{q+1}}({\Bbb D})H^{p,q,s}({\Bbb D}) 的紧算子.

(1) 对任意 f\in H^{\frac{p}{q+1}}({\Bbb D}) , 当-1<q<0 时, 根据 H"{o}lder 不等式, 引理 2.3, C_{\varphi}H^{\frac{p}{q+1}}({\Bbb D}) 上的有界性, 我们可得

\begin{eqnarray*} \| C_{\varphi}f\| _{p,q,s}^{p}&\leq& \sup_{0\leq r<1}\sup_{ a\in {\Bbb D}}(1-r^{2})^{q+s}(1-|a|^{2})^{s} \\ &&\times\left\{\int_{0}^{2\pi}|f[\varphi(r{\rm e}^{{\rm i}\theta})]|^{\frac{p}{q+1}}\ {\rm d}\theta\right\}^{q+1}\left\{\int_{0}^{2\pi}\frac{{\rm d}\theta}{|1- \overline{a}r{\rm e}^{{\rm i}\theta}|^{\frac{2s}{-q}}}\right\}^{-q} \\ &\lesssim &\sup_{0\leq r<1}\sup_{ a\in {\Bbb D}}\frac{(1-r^{2})^{q+s}(1-|a|^{2})^{s}\| f\| ^{p}_{\frac{p}{q+1},0,0}}{(1-r^{2}|a|^{2})^{q+2s}}\lesssim \| f\| ^{p}_{\frac{p}{q+1},0,0}. \end{eqnarray*}

q\geq 0 时, 设 p_{0}=1/(q+1). 由引理 2.6 及 C_{\varphi}H^{pp_{0}}({\Bbb D}) 上的有界性可得

\begin{eqnarray*} \| C_{\varphi}f\| _{p,q,s}^{p}&\leq& \sup_{0\leq r<1}(1-r^{2})^{q}\int_{0}^{2\pi}|f[\varphi(r{\rm e}^{{\rm i}\theta})]|^{p}\ {\rm d}\theta \\ &\leq& \sup_{0\leq r<1}\frac{(1-r^{2})^{q}}{(1-r^{2})^{\frac{1-p_{0}}{p_{0}}}}\| C_{\varphi}f\| _{pp_{0},0,0}^{p}\lesssim\| f\| _{\frac{p}{q+1},0,0}^{p}. \end{eqnarray*}

这表明 C_{\varphi} 总是H^{\frac{p}{q+1}}({\Bbb D})H^{p,q,s}({\Bbb D})的有界算子.

(2) 若 C_{\varphi}H^{\frac{p}{q+1}}({\Bbb D})H^{p,q,s}({\Bbb D}) 的紧算子, 根据(3.10)式可得(3.1)式成立.

(3) 设 \{h_{k}\} 是任一在 {\Bbb D} 的任一紧子集上一致趋于0 且满足\| h_{k}\| _{\frac{p}{q+1},0,0}\leq 1 对所有 k\in \{1,2,\cdots\} 成立的序列. 当 -1<q<0 时, 有

\begin{eqnarray*} \| C_{\varphi}h_{k}\| _{p,q,s}^{p} &\lesssim& \sup_{0\leq r<1}\sup_{ a\in {\Bbb D}}\frac{(1-r^{2})^{q+s}(1-|a|^{2})^{s}}{(1-r^{2}|a|^{2})^{q+2s}}\left\{\int_{0}^{2\pi}|h_{k}[\varphi(r{\rm e}^{{\rm i}\theta})]|^{\frac{p}{q+1}}\ \frac{{\rm d}\theta}{2\pi}\right\}^{q+1} \\ &\leq&\sup_{0\leq r<1}\left\{\int_{0}^{2\pi}|h_{k}[\varphi(r{\rm e}^{{\rm i}\theta})]|^{\frac{p}{q+1}}\ \frac{{\rm d}\theta}{2\pi}\right\}^{q+1}= \| C_{\varphi}h_{k}\| _{\frac{p}{q+1},0,0}^{p}. \end{eqnarray*}

q\geq 0 时, 可得

\| C_{\varphi}h_{k}\| _{p,q,s}^{p} \leq \sup_{0\leq r<1}\frac{(1-r^{2})^{q}}{(1-r^{2})^{\frac{1-p_{0}}{p_{0}}}}\left\{\int_{0}^{2\pi}|h_{k}[\varphi(\sqrt{r}{\rm e}^{{\rm i}\theta})]|^{\frac{p}{q+1}}\ \frac{{\rm d}\theta}{2\pi}\right\}^{q+1}= \| C_{\varphi}h_{k}\| _{\frac{p}{q+1},0,0}^{p}.

如果(3.2)式成立, 根据 Hardy空间的结论有

\lim_{k\rightarrow\infty}\| C_{\varphi}h_{k}\| _{\frac{p}{q+1},0,0}=0. \ \ \mbox{因此,} \ \ \lim_{k\rightarrow\infty}\| C_{\varphi}h_{k}\| _{p,q,s}=0.

这表明 C_{\varphi}H^{\frac{p}{q+1}}({\Bbb D})H^{p,q,s}({\Bbb D}) 的紧算子. 本定理证完.

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