数学物理学报, 2019, 39(1): 15-28 doi:

论文

从混合模空间到Zygmund-型空间的一些积型算子

刘永民,1, 于燕燕,2

On Some Product-Type Operators From Mixed Norm Space to Zygmund-Type Spaces

Liu Yongmin,1, Yu Yanyan,2

通讯作者: 于燕燕, E-mail: minliu@jsnu.edu.cn

收稿日期: 2017-10-25  

基金资助: 国家自然科学基金.  11771184
国家自然科学基金.  11771188
江苏省基础研究计划.  BK20161158

Received: 2017-10-25  

Fund supported: 国家自然科学基金.  11771184
国家自然科学基金.  11771188
江苏省基础研究计划.  BK20161158

作者简介 About authors

刘永民,E-mail:minliu@jsnu.edu.cn , E-mail:minliu@jsnu.edu.cn

摘要

${\mathbb D}=\{ z\in {\mathbb C}: |z|< 1 \}$是复平面上的单位圆盘, $H({\Bbb D})$表示${\Bbb D}$上的所有解析函数的集合, $\psi_1, \psi_2\in H({\Bbb D}),$$n$是一个非负整数, $\varphi$${\Bbb D}$${\Bbb D}$的一个解析自映射, $\mu$是一个权函数.研究从混合模空间到Zygmund-型空间的积型算子$T^n_{\psi_{1},\psi_{2},\varphi}$的有界性和紧性特征,其中

关键词: 积型算子 ; 混合模空间 ; Zygmund-型空间 ; 克兰姆法则

Abstract

Let $H({\Bbb D})$ denote the space of all analytic functions on the unit disk ${\Bbb D}$ in the complex plane $ {\Bbb C}$, $\psi_1, \psi_2\in H({\Bbb D}),$$n$ be a nonnegative integer, $\varphi$ an analytic self-map of $ {\Bbb D}$ and $\mu$ a weight. We study the boundedness and compactness of a product-type operator which is defined by

from the mixed norm space to Zygmund-type spaces.

Keywords: Product-type operator ; Mixed norm space ; Zygmund-type space ; Cramer's Rule

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本文引用格式

刘永民, 于燕燕. 从混合模空间到Zygmund-型空间的一些积型算子. 数学物理学报[J], 2019, 39(1): 15-28 doi:

Liu Yongmin, Yu Yanyan. On Some Product-Type Operators From Mixed Norm Space to Zygmund-Type Spaces. Acta Mathematica Scientia[J], 2019, 39(1): 15-28 doi:

1 引言

${\mathbb D}=\{z\in {\mathbb C}: |z|<1\}$是复平面上的单位圆盘, $H({\Bbb D})$表示${\Bbb D}$上的所有解析函数的集合, $\varphi$${\Bbb D}$${\Bbb D}$的一个解析自映射.

如果存在正数$a$, $b$ ($0< a< b$)$t_0\in[0, 1)$满足

则称$[0, 1)$上的正连续函数$\phi$是一个正规函数.

对于$p, \, q\in (0, \infty)$及正规函数$\phi$,令

其中

$L(p, \, q, \, \phi)$表示${\Bbb D}$上使得$\|f\|_{p, \, q, \, \phi}<\infty$的所有可测函数的集合称为混合模空间. $H(p, \, q, \, \phi)$$=L(p, \, q, \, \phi)\cap H({\Bbb D})$.$1\leq p<\infty$时, $H(p, \, q, \, \phi)$是以$\|\cdot\|_{p, \, q, \, \phi}$为范数的Banach空间;当$0<p<1$时, $H(p, \, q, \, \phi)$是以$\|\cdot\|_{p, \, q, \, \phi}$为半范数的Fréchet空间,但不是Banach空间.

$\mu$是一个权函数,即${\Bbb D}$上的正连续函数.令

$f\in H({\Bbb D})$$\|f\|_{{\cal Z}_{\mu}}<\infty$,则称$f$属于Zygmund-型空间${{\mathcal Z}_\mu}$. $({{\mathcal Z}_\mu}, \|\cdot\|_{{\cal Z}_{\mu}})$也是一个Banach空间.如果$\mu(z)=1-|z|^2$, Zygmund-型空间${\cal Z}_{\mu}$就是经典的Zygmund空间${\mathcal Z}$.

近年来,人们在研究混合模空间与Zygmund-型空间之间某些算子的性质,参见论文[1-13]及它们中的参考文献.对于单位球上全纯函数空间上某些算子的研究参见文献[14-20].

最近, Stević, Sharma及Krishan在文献[21]中引入算子

其中$\psi_1, \psi_2\in H({\Bbb D}), $$n$是非负整数, $\varphi$${\Bbb D}$${\Bbb D}$的一个解析自映射.他们研究了从一般空间到Bloch-型空间$T^n_{\psi_{1}, \psi_{2}, \varphi}$的有界性与紧性.对$\psi_2\equiv0$,可以得到加权微分复合算子,它的研究见论文[22-28].当$n=0$时, $T^n_{\psi_{1}, \psi_{2}, \varphi}=T_{\psi_{1}, \psi_{2}, \varphi}$,后者是由Stević等在文献[29]中引进的.

受论文[16, 21, 24, 26, 30-31]的启发,本文研究算子$T^n_{\psi_{1}, \psi_{2}, \varphi}: H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$的有界性与紧性特征.

2 预备知识

先给出一些预备知识.

引理2.1[32]  设$p, q \in (0, \infty)$, $\phi$是正规的且$f\in H(p, q, \phi)$.则对于$n\in{\mathbb N}_0$,存在一个与$f$无关的常数$C$使得

下面的紧性准则是有用的工具,它的证明可以参见文献[33]中的命题3.11.

引理2.2  设$\psi_1, \psi_2\in H({\Bbb D})$, $n\in{\mathbb N}_0$, $\varphi$${\Bbb D}$${\Bbb D}$的一个解析自映射, $\mu$是一个权函数.则$T^n_{\psi_{1}, \psi_{2}, \varphi}:H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是紧的充要条件$T^n_{\psi_{1}, \psi_{2}, \varphi}: H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是有界的且对于在${\Bbb D}$的任意紧子集上一致收敛于零($k\rightarrow \infty$)的有界序列$\{f_k\}\subset H(p, q, \phi)$,有$\|T^n_{\psi_{1}, \psi_{2}, \varphi}f_k\|_{{\cal Z}_{_{\mu}}}\rightarrow 0\ (k\rightarrow \infty)$.

引理2.3[34]  对任意的实数$\beta$,设

引理2.4[35]  对于$\beta>-1$$\gamma> 1+\beta$,则

3 算子$T^n_{\psi_{1}, \psi_{2}, \varphi}:H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$的有界性与紧性

本节将给出我们的主要结果与证明.

定理3.1  设$\psi_1, \psi_2\in H({\Bbb D})$, $n\in{\mathbb N}_0$, $\varphi$${\Bbb D}$${\Bbb D}$的一个解析自映射, $\mu$是一个权函数.则$T^n_{\psi_{1}, \psi_{2}, \varphi}:H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是有界的充要条件

$\begin{equation} \label{qwe1}\sup\limits_{z\in{\Bbb D}}\frac{\mu(z)|\psi_1''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n}}<\infty, \end{equation}$

$\begin{equation}\label{qwe2}\sup\limits_{z\in{\Bbb D}}\frac{\mu(z)|\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+1}}<\infty, \end{equation}$

$\begin{equation}\label{qwe3}\sup\limits_{z\in{\Bbb D}}\frac{\mu(z)|\psi_1(z)(\varphi'(z))^2+2\psi_2'(z)\varphi'(z)+\psi_2(z)\varphi''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+2}}<\infty, \end{equation}$

$\begin{equation}\label{qwe3b}\sup\limits_{z\in{\Bbb D}}\frac{\mu(z)|\psi_2(z)||\varphi'(z)|^2}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+3}}<\infty.\end{equation}$

  充分性.假设(3.1)-(3.4)式成立.由于

因此对$z\in{\Bbb D}$$f\in H(p, q, \phi)$,根据引理2.1,我们有

$\begin{eqnarray}\label{qwe4} &&\mu(z)\left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f\right)^{''}(z)\right|\nonumber\\&\leq&\mu(z)|\psi_1''(z)||f^{(n)}(\varphi(z))|+\mu(z)\left|\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z)\right|\left|f^{(n+1)}(\varphi(z))\right|\nonumber\\&& +\mu(z)|\psi_1(z)(\varphi'(z))^2+2\psi_2'(z)\varphi'(z)+\psi_2(z)\varphi''(z)|\left|f^{(n+2)}(\varphi(z))\right|\nonumber\\&& +\mu(z)\left|\psi_2(z)(\varphi'(z))^2\right|\left|f^{(n+3)}(\varphi(z))\right|\nonumber\\&\leq& C\|f\|_{p, q, \phi}\frac{\mu(z)|\psi_1''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n}}+C\|f\|_{{\cal B}_{\log}}\frac{\mu(z)|\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+1}}\nonumber\\&& +C\|f\|_{p, q, \phi}\frac{\mu(z)\left|\psi_1(z)(\varphi'(z))^2+2\psi_2'(z)\varphi'(z)+\psi_2(z)\varphi''(z)\right|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+2}}\nonumber\\&& +C\|f\|_{p, q, \phi}\frac{\mu(z)|\psi_2(z)||\varphi'(z)|^2}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+3}}\nonumber\\&\leq& C\|f\|_{p, q, \phi}.\end{eqnarray}$

另一方面

$\begin{eqnarray}\label{qwe5}\left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f\right)(0)\right|&=&\left|\psi_1(0)f^{(n)}(\varphi(0))+\psi_2(0)f^{(n+1)}(\varphi(0))\right|\nonumber\\&\leq&C\frac{|\psi_1(0)|+|\psi_2(0)|}{\phi(|\varphi(0)|)\left(1-\left|\varphi(0)\right|^{2}\right)^{1/q+n+1}}\|f\|_{p, q, \phi}, \end{eqnarray}$

$\begin{eqnarray}\label{qwe6}&&\left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f\right)'(0)\right|\nonumber\\&=&\left|\psi_1'(0)f^{(n)}(\varphi(0))+(\psi_1(0)\varphi'(0)+\psi_2'(0))f^{(n+1)}(\varphi(0))+\psi_2(0)\varphi'(0)f^{(n+2)}(\varphi(0))\right|\nonumber\\&\leq&C\frac{|\psi_1'(0)|+|\psi_1(0)\varphi'(0)+\psi_2'(0)|+|\psi_2(0)\varphi'(0)|}{\phi(|\varphi(0)|)\left(1-\left|\varphi(0)\right|^{2}\right)^{1/q+n+2}}\|f\|_{p, q, \phi}.\end{eqnarray}$

利用(3.5), (3.6)及(3.7)式,我们得到算子$T^n_{\psi_{1}, \psi_{2}, \varphi}:H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是有界的.

必要性.设$T^n_{\psi_{1}, \psi_{2}, \varphi}: H(p, q, \phi)\rightarrow\mathcal{Z}_{\mu} $是有界的,则存在常数$C$使得

$\begin{equation}\label{qweyou}\|T^n_{\psi_{1}, \psi_{2}, \varphi}f\|_{{\cal Z}_{\mu}}\leq C\|f\|_{p, q, \phi}, \end{equation}$

对任意$f\in H(p, q, \phi)$.在(3.8)式中取$f(z)=\frac{z^{n}}{n!} \in H(p, q, \phi)$,我们有

$\begin{equation}\label{qwe7} K_{1}:=\sup\limits_{z\in{\Bbb D}}\mu(z)|\psi_1''(z)|<\infty.\end{equation}$

在(3.8)式中取$f(z)=\frac{z^{n+1}}{(n+1)!} \in H(p, q, \phi)$,可得

$\begin{equation}\label{qwe8} \sup\limits_{z\in{\Bbb D}}\mu(z)|\psi_1''(z)\varphi(z)+\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z)|<\infty.\end{equation}$

由于(3.9)式, (3.10)式以及函数$\varphi(z)$是有界的,所以

$\begin{equation}\label{qwe9} K_{2}:=\sup\limits_{z\in{\Bbb D}}\mu(z)|\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z)|<\infty.\end{equation}$

再在(3.8)式中取$f(z)=\frac{z^{n+2}}{(n+2)!} \in H(p, q, \phi)$,又可得到

$\begin{eqnarray}\label{qwe10} &&\sup\limits_{z\in{\Bbb D}}\mu(z)\Big|\frac{1}{2}\psi_1''(z)(\varphi(z))^2+(\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z))\varphi(z)\nonumber\\&& +(\psi_1(z)(\varphi'(z))^2+2\psi_2'(z)\varphi'(z)+\psi_2(z)\varphi''(z)) \Big|<\infty.\end{eqnarray}$

利用(3.9), (3.11)和(3.12)式及$\varphi(z)$的有界性,最后得到

$\begin{equation}\label{qwe11} K_{3}:=\sup\limits_{z\in{\Bbb D}}\mu(z)\left|\psi_1(z)(\varphi'(z))^2+2\psi_2'(z)\varphi'(z)+\psi_2(z)\varphi''(z)\right|<\infty.\end{equation}$

类似可得

$\begin{equation} \label{qwe11b} K_{4}:=\sup\limits_{z\in{\Bbb D}}\mu(z)|\psi_2(z)||\varphi'(z)|^2<\infty.\end{equation}$

对固定的$w\in{\Bbb D}$以及常数$A, B, C$,令

$\begin{equation}\label{qwe12} f_{w}(z)=\frac{(1-|w|^2)^{b+1}}{\phi(|w|)}\left(\frac{1}{(1-\overline{w}z)^{\alpha}}+A\frac{(1-|w|^2)}{(1-\overline{w}z)^{\alpha+1}}+ B\frac{(1-|w|^2)^2}{(1-\overline{w}z)^{\alpha+2}} +C\frac{(1-|w|^2)^3}{(1-\overline{w}z)^{\alpha+3}}\right), \end{equation}$

其中$b$由函数$\phi$确定且$\alpha=1/q+b+1$.简单计算可得

$\begin{eqnarray}\label{qwe13}f^{(n)}_{w}(z)&=&\frac{(1-|w|^2)^{b+4}(\overline{w})^n}{\phi(|w|)(1-\overline{w}z)^{\alpha+n}}\left(\frac{\alpha\cdots(\alpha+n-1)}{(1-|w|^2)^3}+\frac{A(\alpha+1)\cdots(\alpha+n)}{(1-|w|^2)^2(1-\overline{w}z)}\right.\nonumber\\&&+\left.\frac{B(\alpha+2)\cdots(\alpha+n+1)}{(1-|w|^2)(1-\overline{w}z)^2} +\frac{C(\alpha+3)\cdots(\alpha+n+2)}{(1-\overline{w}z)^3}\right);\end{eqnarray}$

$\begin{eqnarray}\label{qwe14}f^{(n+1)}_{w}(z)&=&\frac{(1-|w|^2)^{b+4}(\overline{w})^{n+1}}{\phi(|w|)(1-\overline{w}z)^{\alpha+n+1}}\left(\frac{\alpha\cdots(\alpha+n)}{(1-|w|^2)^3}+\frac{A(\alpha+1)\cdots(\alpha+n+1)}{(1-|w|^2)^2(1-\overline{w}z)}\right.\nonumber\\&&+\left.\frac{B(\alpha+2)\cdots(\alpha+n+2)}{(1-|w|^2)(1-\overline{w}z)^2} +\frac{C(\alpha+3)\cdots(\alpha+n+3)}{(1-\overline{w}z)^3}\right);\end{eqnarray}$

$\begin{eqnarray}\label{qwe15}f^{(n+2)}_{w}(z)&=&\frac{(1-|w|^2)^{b+4}(\overline{w})^{n+2}}{\phi(|w|)(1-\overline{w}z)^{\alpha+n+2}}\left(\frac{\alpha\cdots(\alpha+n+1)}{(1-|w|^2)^3}+\frac{A(\alpha+1)\cdots(\alpha+n+2)}{(1-|w|^2)^2(1-\overline{w}z)}\right.\nonumber\\&&+\left.\frac{B(\alpha+2)\cdots(\alpha+n+3)}{(1-|w|^2)(1-\overline{w}z)^2} +\frac{C(\alpha+3)\cdots(\alpha+n+4)}{(1-\overline{w}z)^3}\right);\end{eqnarray}$

$\begin{eqnarray} \label{qwe15b}f^{(n+3)}_{w}(z)&=&\frac{(1-|w|^2)^{b+4}(\overline{w})^{n+3}}{\phi(|w|)(1-\overline{w}z)^{\alpha+n+3}}\left(\frac{\alpha\cdots(\alpha+n+2)}{(1-|w|^2)^3}+\frac{A(\alpha+1)\cdots(\alpha+n+3)}{(1-|w|^2)^2(1-\overline{w}z)}\right.\nonumber\\&&+\left.\frac{B(\alpha+2)\cdots(\alpha+n+4)}{(1-|w|^2)(1-\overline{w}z)^2} +\frac{C(\alpha+3)\cdots(\alpha+n+5)}{(1-\overline{w}z)^3}\right);\end{eqnarray}$

利用引理2.3,可得

$\begin{eqnarray}\label{qwee123} &&M_q(f_w, r)\leq C\frac{(1-|w|^2)^{b+1}}{\phi(|w|)(1-r|w|)^{b+1}}. \end{eqnarray}$

根据$\phi$的正规性及引理2.4,可得(参见文献[26, 32])

$\begin{eqnarray}\label{eq10} \sup\limits_{w\in \rm {\Bbb D}}\|f_w\|_{p, q, \phi}\leq C.\end{eqnarray}$

为证明我们的结果,首先考察方程组

$\begin{eqnarray}\label{sys1} && \alpha\cdots(\alpha+n) +A(\alpha+1)\cdots(\alpha+n+1)\nonumber \\ &&+B(\alpha+2)\cdots(\alpha+n+2)+C(\alpha+3)\cdots(\alpha+n+3)=0, \nonumber \\ && \alpha\cdots(\alpha+n+1) +A(\alpha+1)\cdots(\alpha+n+2)\nonumber \\ &&+B(\alpha+2)\cdots(\alpha+n+3)+C(\alpha+3)\cdots(\alpha+n+4)=0, \\ && \alpha\cdots(\alpha+n+2) +A(\alpha+1)\cdots(\alpha+n+3)\nonumber \\ &&+B(\alpha+2)\cdots(\alpha+n+4)+C(\alpha+3)\cdots(\alpha+n+5)=0.\nonumber\end{eqnarray}$

方程组(3.22)变形为

$\begin{eqnarray} \label{sys2} && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n+1)\nonumber \\ &&+B(\alpha+2)(\alpha+n+1)(\alpha+n+2)+C(\alpha+n+1)(\alpha+n+2)(\alpha+n+3)=0, \nonumber \\ && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n+2)\nonumber \\ &&+B(\alpha+2)(\alpha+n+2)(\alpha+n+3)+C(\alpha+n+2)(\alpha+n+3)(\alpha+n+4)=0, \\ && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n+3)\nonumber \\ &&+B(\alpha+2)(\alpha+n+3)(\alpha+n+4)+C(\alpha+n+3)(\alpha+n+4)(\alpha+n+5)=0.\nonumber\end{eqnarray}$

由于方程组(3.23)的系数行列式

根据克兰姆法则,方程组(3.23)有非零解.由(3.16)-(3.19)式,存在常数$A, B, C$使得$f_{w}^{(n+1)}(w)=f_{w}^{(n+2)}(w)=f_{w}^{(n+3)}(w)=0$

其中$C_1(A, B, C, \alpha, n)=\alpha\cdots(\alpha+n-1) +A(\alpha+1)\cdots(\alpha+n) +B(\alpha+2)\cdots(\alpha+n+1)+C(\alpha+3)\cdots(\alpha+n+2)\neq 0$.因此对$\omega\in {\Bbb D}$$\varphi(\omega)\neq 0$,取检验函数$f_{\varphi(\omega)}$,我们得到

$\begin{eqnarray}\label{qwe16}C&\geq&\|T^n_{\psi_{1}, \psi_{2}, \varphi}f_{\varphi(\omega)}\|_{{\cal Z}_{\mu}}\geq \mu(\omega)\left|\psi_1''(\omega)f^{(n)}_{\varphi(\omega)}(\varphi(\omega))\right|\nonumber\\&=&|C_1(A, B, C, \alpha, n)|\frac{\mu(\omega)|\psi_1''(\omega)|\left|\overline{\varphi(\omega)}\right|^{n}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n}}.\end{eqnarray}$

由(3.24)式,对$r\in(t_0, 1)$,有

$\begin{eqnarray}\label{qwe18}\sup\limits_{r<|\varphi(\omega)|<1}\frac{\mu(\omega)|\psi_1''(\omega)|}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n}}&\leq& \frac{1}{r^n}\sup\limits_{r<|\varphi(\omega)|<1}\frac{\mu(\omega)|\psi_1''(\omega)|\left|\overline{\varphi(\omega)}\right|^{n}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n}}\nonumber\\&\leq& \frac{1}{r^n}\sup\limits_{\omega\in{\Bbb D}}\frac{\mu(\omega)|\psi_1''(\omega)|\left|\overline{\varphi(\omega)}\right|^{n}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n}}\nonumber\\&\leq &C<\infty.\end{eqnarray}$

又从(3.9)式可得

$\begin{eqnarray}\label{qwe17}\sup\limits_{|\varphi(\omega)|\leq r}\frac{\mu(\omega)|\psi_1''(\omega)|}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n}}\leq C\sup\limits_{|\varphi(\omega)|\leq r}\mu(\omega)|\psi_1''(\omega)|\leq CK_{1}<\infty.\end{eqnarray}$

因此把(3.26)与(3.25)式结合起来可得(3.1)式成立.

其次考察方程组

$ \begin{eqnarray}\label{sys3} && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n)\nonumber \\ &&+B(\alpha+2)(\alpha+n)(\alpha+n+1)+C(\alpha+n)(\alpha+n+1)(\alpha+n+2)=0, \nonumber \\ && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n+2)\nonumber \\ &&+B(\alpha+2)(\alpha+n+2)(\alpha+n+3)+C(\alpha+n+2)(\alpha+n+3)(\alpha+n+4)=0, \\ && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n+3)\nonumber \\ &&+B(\alpha+2)(\alpha+n+3)(\alpha+n+4)+C(\alpha+n+3)(\alpha+n+4)(\alpha+n+5)=0.\nonumber \end{eqnarray}$

由于

根据克兰姆法则,方程组(3.27)有非零解.由(3.16)-(3.19)式,知在(3.15)式中存在常数$A, B, C$使得$g_{w}^{(n)}(w)=g_{w}^{(n+2)}(w)=g_{w}^{(n+3)}(w)=0$

其中$C_2(A, B, C, \alpha, n)=\alpha\cdots(\alpha+n) +A(\alpha+1)\cdots(\alpha+n+1) +B(\alpha+2)\cdots(\alpha+n+2)+C(\alpha+3)\cdots(\alpha+n+3)\neq 0$, $g_{w}$表示相应的函数.因此对$\omega\in {\Bbb D}$$\varphi(\omega)\neq 0$,考察检验函数$g_{\varphi(\omega)}$,可得

$\begin{eqnarray}\label{qwe23}C&\geq&\|T^n_{\psi_{1}, \psi_{2}, \varphi}g_{\varphi(\omega)}\|_{{\cal Z}_{\mu}}\nonumber\\&\geq&\mu(\omega)\left|\psi_1(\omega)\varphi''(\omega)+2\psi_1'(\omega)\varphi'(\omega)+\psi_2''(\omega)\right|\left|g^{(n+1)}_{\varphi(\omega)}(\varphi(\omega))\right|\nonumber\\&=&|C_2(A, B, C, \alpha, n)|\frac{\mu(\omega)\left|\psi_1(\omega)\varphi''(\omega)+2\psi_1'(\omega)\varphi'(\omega)+\psi_2''(\omega)\right|\left|\overline{\varphi(\omega)}\right|^{n+1}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+1}}.\end{eqnarray}$

利用(3.28)式有

$\begin{eqnarray}\label{qwe24}&&\sup\limits_{r<|\varphi(\omega)|<1}\frac{\mu(\omega)|\psi_1(\omega)\varphi''(\omega)+2\psi_1'(\omega)\varphi'(\omega)+\psi_2''(\omega)|}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+1}}\nonumber\\&\leq &\frac{1}{r^{n+1}}\sup\limits_{r<|\varphi(\omega)|<1} \frac{\mu(\omega)|\psi_1(\omega)\varphi''(\omega)+2\psi_1'(\omega)\varphi'(\omega)+\psi_2''(\omega)|\left|\overline{\varphi(\omega)}\right|^{n+1}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+1}}\nonumber\\&\leq &\frac{1}{r^{n+1}}\sup\limits_{\omega\in{\Bbb D}} \frac{\mu(\omega)|\psi_1(\omega)\varphi''(\omega)+2\psi_1'(\omega)\varphi'(\omega)+\psi_2''(\omega)|\left|\overline{\varphi(\omega)}\right|^{n+1}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+1}}\nonumber\\ &\leq& C <\infty.\end{eqnarray}$

根据(3.11)式,我们可得

$\begin{eqnarray}\label{qwe25}&&\sup\limits_{|\varphi(\omega)|\leq r}\frac{\mu(\omega)|\psi_1(\omega)\varphi''(\omega)+2\psi_1'(\omega)\varphi'(\omega)+\psi_2''(\omega)|}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+1}}\nonumber\\&\leq &C\sup\limits_{|\varphi(\omega)|\leq r}\mu(\omega)|\psi_1(\omega)\varphi''(\omega)+2\psi_1'(\omega)\varphi'(\omega)+\psi_2''(\omega)|\nonumber\\&\leq& CK_{2}<\infty.\end{eqnarray}$

由(3.29)及(3.30)式可得(3.2)式成立.

再次为了证明(3.3)式,可考察方程组

$\begin{eqnarray}\label{sys4}&& \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n)\nonumber \\ &&+B(\alpha+2)(\alpha+n)(\alpha+n+1)+C(\alpha+n)(\alpha+n+1)(\alpha+n+2)=0, \nonumber \\ && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n+1)\nonumber \\ &&+B(\alpha+2)(\alpha+n+1)(\alpha+n+2)+C(\alpha+n+1)(\alpha+n+2)(\alpha+n+3)=0, \\ && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n+3)\nonumber \\ &&+B(\alpha+2)(\alpha+n+3)(\alpha+n+4)+C(\alpha+n+3)(\alpha+n+4)(\alpha+n+5)=0.\nonumber \end{eqnarray}$

由于

由(3.16)-(3.19)式可知,存在(3.15)式中的常数$A, B, C$使得$h_{w}^{(n)}(w)=h_{w}^{(n+1)}(w)=h_{w}^{(n+3)}(w)=0$

这里$C_3(A, B, C, \alpha, n)=\alpha\cdots(\alpha+n+1) +A(\alpha+1)\cdots(\alpha+n+2) +B(\alpha+2)\cdots(\alpha+n+3)+C(\alpha+3)\cdots(\alpha+n+4)\neq 0$, $h_{w}$表示相应的函数.因此对$\omega\in {\Bbb D}$$\varphi(\omega)\neq 0$,考察检验函数$h_{\varphi(\omega)}$,可得

$\begin{eqnarray}\label{qwe30}C&\geq&\|T^n_{\psi_{1}, \psi_{2}, \varphi}h_{\varphi(\omega)}\|_{{\cal Z}_{\mu}}\nonumber\\&\geq&\mu(\omega)|\psi_1(\omega)(\varphi'(\omega))^2+2\psi_2'(\omega)\varphi'(\omega)+\psi_2(\omega)\varphi''(\omega)|\left|h^{(n+2)}_{\varphi(\omega)}(\varphi(\omega))\right|\nonumber\\&=&|C_4(A, B, C, \alpha, n)|\frac{\mu(\omega)|\psi_1(\omega)(\varphi'(\omega))^2+2\psi_2'(\omega)\varphi'(\omega)+\psi_2(\omega)\varphi''(\omega)|\left|\overline{\varphi(\omega)}\right|^{n+2}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+2}}.\nonumber\\\end{eqnarray}$

利用(3.32)式,对$r\in(t_0, 1)$,有

$\begin{eqnarray}\label{qwe31}&&\sup\limits_{r<|\varphi(\omega)|<1}\frac{\mu(\omega)\left|\psi_1(\omega)(\varphi'(\omega))^2+2\psi_2'(\omega)\varphi'(\omega)+\psi_2(\omega)\varphi''(\omega)\right|}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+2}}\nonumber\\&\leq&\frac{1}{r^{n+2}}\sup\limits_{r<|\varphi(\omega)|<1}\frac{\mu(\omega)|\psi_1(\omega)(\varphi'(\omega))^2+2\psi_2'(\omega)\varphi'(\omega)+\psi_2(\omega)\varphi''(\omega)|\left|\overline{\varphi(\omega)}\right|^{n+2}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+2}}\nonumber\\&\leq& \frac{1}{r^{n+2}}\sup\limits_{\omega\in{\Bbb D}}\frac{\mu(\omega)|\psi_1(\omega)(\varphi'(\omega))^2+2\psi_2'(\omega)\varphi'(\omega)+\psi_2(\omega)\varphi''(\omega)|\left|\overline{\varphi(\omega)}\right|^{n+2}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+2}}\nonumber\\&\leq& C<\infty.\end{eqnarray}$

使用(3.13)式,我们有

$\begin{eqnarray}\label{qwe32}&&\sup\limits_{|\varphi(\omega)|\leq r}\frac{\mu(\omega)|\psi_1(\omega)(\varphi'(\omega))^2+2\psi_2'(\omega)\varphi'(\omega)+\psi_2(\omega)\varphi''(\omega)|}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+2}}\nonumber\\&\leq&\sup\limits_{|\varphi(\omega)|\leq r}\mu(\omega)|\psi_1(\omega)(\varphi'(\omega))^2+2\psi_2'(\omega)\varphi'(\omega)+\psi_2(\omega)\varphi''(\omega)|\nonumber\\&\leq& CK_{3}<\infty.\end{eqnarray}$

依据(3.33)和(3.34)式, (3.3)式成立.

最后我们证明(3.4)式成立.为此考察下面的方程组

$ \begin{eqnarray} && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n)\nonumber \\ &&+B(\alpha+2)(\alpha+n)(\alpha+n+1)+C(\alpha+n)(\alpha+n+1)(\alpha+n+2)=0, \nonumber \\ && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n+1)\nonumber \\ &&+B(\alpha+2)(\alpha+n+1)(\alpha+n+2)+C(\alpha+n+1)(\alpha+n+2)(\alpha+n+3)=0, \\ && \alpha(\alpha+1)(\alpha+2) +A(\alpha+1)(\alpha+2)(\alpha+n+2)\nonumber \\ &&+B(\alpha+2)(\alpha+n+2)(\alpha+n+3)+C(\alpha+n+2)(\alpha+n+3)(\alpha+n+4)=0.\nonumber \end{eqnarray}$

由于

从(3.16)-(3.19)式,知在(3.15)式中一定存在$A, B, C$使得$k_{w}^{(n)}(w)=k_{w}^{(n+1)}(w)=k_{w}^{(n+2)}(w)=0$

其中$C_4(A, B, C, \alpha, n)=\alpha\cdots(\alpha+n+2) +A(\alpha+1)\cdots(\alpha+n+3) +B(\alpha+2)\cdots(\alpha+n+4)+C(\alpha+3)\cdots(\alpha+n+5)\neq 0$, $k_{w}$表示相应的函数.因此对$\omega\in {\Bbb D}$$\varphi(\omega)\neq 0$,对检验函数$k_{\varphi(\omega)}$,有

$\begin{eqnarray}\label{qwe30b}C&\geq&\|T^n_{\psi_{1}, \psi_{2}, \varphi}k_{\varphi(\omega)}\|_{{\cal Z}_{\mu}}\nonumber\\&\geq&\mu(\omega)|\psi_2(\omega)||\varphi'(\omega)|^2\left|k^{(n+3)}_{\varphi(\omega)}(\varphi(\omega))\right|\nonumber\\&=&|C_4(A, B, C, \alpha, n)|\frac{\mu(\omega)|\psi_2(\omega)||\varphi'(\omega)|^2\left|\overline{\varphi(\omega)}\right|^{n+3}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+3}}.\end{eqnarray}$

由(3.36)式,得到

$\begin{eqnarray}\label{qwe31b}\sup\limits_{r<|\varphi(\omega)|<1}\frac{\mu(\omega)|\psi_2(\omega)||\varphi'(\omega)|^2}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+3}}&\leq&\frac{1}{r^{n+3}}\sup\limits_{r<|\varphi(\omega)|<1}\frac{\mu(\omega)|\psi_2(\omega)||\varphi'(\omega)|^2\left|\overline{\varphi(\omega)}\right|^{n+3}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+3}}\nonumber\\&\leq &\frac{1}{r^{n+3}}\sup\limits_{\omega\in{\Bbb D}}\frac{\mu(\omega)|\psi_2(\omega)||\varphi'(\omega)|^2\left|\overline{\varphi(\omega)}\right|^{n+3}}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+3}}\nonumber\\&\leq &C<\infty.\end{eqnarray}$

另一方面由(3.14)式知

$\begin{eqnarray}\label{qwe32b}\sup\limits_{|\varphi(\omega)|\leq r}\frac{\mu(\omega)|\psi_2(\omega)||\varphi'(\omega)|^2}{\phi(|\varphi(\omega)|)\left(1-\left|\varphi(\omega)\right|^{2}\right)^{1/q+n+3}}&\leq&\sup\limits_{|\varphi(\omega)|\leq r} C\mu(\omega)|\psi_2(\omega)||\varphi'(\omega)|^2\\&\leq& CK_{4}<\infty.\end{eqnarray}$

结合(3.37)和(3.38)式即可推出(3.4)式成立,注意在我们的证明中,我们已经使用了以下事实:对固定的$\omega\in{\Bbb D}$$\varphi(\omega)\neq 0$,函数$g_{\varphi(\omega)}, h_{\varphi(\omega)}, k_{\varphi(\omega)}\in H(p, q, \phi)$.证毕.

定理3.2  设$\psi_1, \psi_2\in H({\Bbb D})$, $n\in{\mathbb N}_0$, $\varphi$${\Bbb D}$${\Bbb D}$的一个解析自映射, $\mu$是一个权函数,则$T^n_{\psi_{1}, \psi_{2}, \varphi}:H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是紧的充要条件$T^n_{\psi_{1}, \psi_{2}, \varphi}:H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是有界的,

$\begin{equation}\label{qwe33}\lim\limits_{|\varphi(z)|\rightarrow1}\frac{\mu(z)|\psi_1''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n}}=0, \end{equation}$

$\begin{equation}\label{qwe34}\lim\limits_{|\varphi(z)|\rightarrow1}\frac{\mu(z)|\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+1}}=0, \end{equation}$

$\begin{equation}\label{qwe35}\lim\limits_{|\varphi(z)|\rightarrow1}\frac{\mu(z)|\psi_1(z)(\varphi'(z))^2+2\psi_2'(z)\varphi'(z)+\psi_2(z)\varphi''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+2}}=0, \end{equation}$

$\begin{equation} \label{qwe35b}\lim\limits_{|\varphi(z)|\rightarrow1}\frac{\mu(z)|\psi_2(z)||\varphi'(z)|^2}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+3}}=0.\end{equation}$

  充分性.设$T^n_{\psi_{1}, \psi_{2}, \varphi}: H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是有界的且条件(3.39)-(3.42)式成立.对于在${\Bbb D}$的任意紧子集上一致收敛于零($k\rightarrow \infty$)的有界序列$\{f_k\}\subset H(p, q, \phi)$,根据引理2.2,只需证明

不失一般性不妨设$\|f_{k}\|_{p, q, \phi}\leq1$.由(3.39)-(3.42)式,对任意的$\varepsilon>0$,一定存在$\rho \in(0, 1)$,当$ \rho<|\varphi(z)|<1$时,有

$\begin{equation}\label{qwe36} \frac{\mu(z)|\psi_1''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n}}<\varepsilon, \end{equation}$

$\begin{equation}\label{qwe37}\frac{\mu(z)|\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+1}}<\varepsilon, \end{equation}$

$\begin{equation}\label{qwe38}\frac{\mu(z)|\psi_1(z)(\varphi'(z))^2+2\psi_2'(z)\varphi'(z)+\psi_2(z)\varphi''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+2}}<\varepsilon, \end{equation}$

$\begin{equation} \label{qwe38b}\frac{\mu(z)|\psi_2(z)||\varphi'(z)|^2}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+3}}<\varepsilon.\end{equation}$

由于算子$T^n_{\psi_{1}, \psi_{2}, \varphi}: H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是有界的,根据定理3.1,我们看到(3.9), (3.11), (3.13)及(3.14)式成立.又因为$f_{k}$${\Bbb D}$的任意紧子集上一致收敛于零($k\rightarrow \infty$), Cauchy估计保证$f^{(n)}_{k}$, $f^{(n+1)}_{k}$, $f^{(n+2)}_{k}$$f^{(n+3)}_{k}$${\Bbb D}$的任意紧子集上也一致收敛于零,于是存在常数$K_{0}\in{\Bbb N}$使得当$k>K_{0}$时,对$\rho\in(0, 1)$,有

$\begin{eqnarray}\label{qwe39}&&|(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k})(0)|+|(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k})'(0)|+\sup\limits_{|\varphi(z)|\leq\rho}\mu(z)\left|(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k})''(z)\right|\nonumber\\&\leq&|\psi_1(0)|\left|f^{(n)}_{k}(\varphi(0))\right|+\left|\psi_2(0)f^{(n+1)}_{k}(\varphi(0))\right|+\left|\psi'(0)||f^{(n)}_{k}(\varphi(0))\right|\nonumber\\&& +|\psi(0)\varphi'(0)|\left|f^{(n+1)}_{k}(\varphi(0))\right|+\left|\psi_2(0)\varphi'(0)f^{(n+2)}_{k}(\varphi(0))\right|\nonumber\\&& +\sup\limits_{|\varphi(z)|\leq\rho}\mu(z)\left|\psi_1''(z)||f^{(n)}_{k}(\varphi(z))\right|\nonumber\\&& +\sup\limits_{|\varphi(z)|\leq\rho}\mu(z)|\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z)|\left|f^{(n+1)}_{k}(\varphi(z))\right|\nonumber\\&& +\sup\limits_{|\varphi(z)|\leq\rho}\mu(z)|\psi_1(z)(\varphi'(z))^2+2\psi_2'(z)\varphi'(z)+\psi_2(z)\varphi''(z)|\left|f^{(n+2)}_{k}(\varphi(z))\right|\nonumber\\&& +\sup\limits_{|\varphi(z)|\leq\rho}\mu(z)|\psi_2(z)||\varphi'(z)|^2\left|f^{(n+3)}_{k}(\varphi(z))\right|\nonumber\\&\leq& C\varepsilon +K_{1}\sup\limits_{|\varphi(z)|\leq\rho}\left|f^{(n)}_{k}(\varphi(z))\right|+K_{2}\sup\limits_{|\varphi(z)|\leq\rho}\left|f^{(n+1)}_{k}(\varphi(z))\right|\nonumber\\&& +K_{3}\sup\limits_{|\varphi(z)|\leq\rho}|f^{(n+2)}_{k}(\varphi(z))|+K_{4}\sup\limits_{|\varphi(z)|\leq\rho}|f^{(n+3)}_{k}(\varphi(z))|\nonumber\\&<&C\varepsilon.\end{eqnarray}$

利用(3.43)-(3.47)式以及引理2.1,可得当$k>K_{0}$

$\begin{eqnarray}\label{qwe40}\|T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k}\|_{\mathcal{Z}_{\mu}}&=&\left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k}\right)(0)\right|+\left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k}\right)'(0)\right|+\sup\limits_{z\in{\Bbb D}}\mu(z)\left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k}\right)^{''}(z)\right|\nonumber\\&\leq& \left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k}\right)(0)\right|+\left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k}\right)'(0)\right|\nonumber\\&&+\sup\limits_{|\varphi(z)|\leq\rho}\mu(z)\left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k}\right)^{''}(z)\right|+\sup\limits_{\rho<|\varphi(z)|<1}\mu(z)\left|\left(T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k}\right)^{''}(z)\right|\nonumber\\&<&C\varepsilon+C\sup\limits_{\rho<|\varphi(z)|<1}\frac{\mu(z)|\psi_1''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n}}\|f\|_{p, q, \phi}\nonumber\\&& +C\sup\limits_{\rho<|\varphi(z)|<1}\frac{\mu(z)|\psi_1(z)\varphi''(z)+2\psi_1'(z)\varphi'(z)+\psi_2''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+1}}\|f\|_{p, q, \phi}\nonumber\\&& +C\sup\limits_{\rho<|\varphi(z)|<1}\frac{\mu(z)|\psi_1(z)(\varphi'(z))^2+2\psi_2'(z)\varphi'(z)+\psi_2(z)\varphi''(z)|}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+2}}\|f\|_{p, q, \phi} \nonumber\\&& +C\sup\limits_{\rho<|\varphi(z)|<1}\frac{\mu(z)|\psi_2(z)||\varphi'(z)|^2}{\phi(|\varphi(z)|)\left(1-\left|\varphi(z)\right|^{2}\right)^{1/q+n+3}}\|f\|_{p, q, \phi} \nonumber\\&<&4C\varepsilon.\end{eqnarray}$

因此算子$T^n_{\psi_{1}, \psi_{2}, \varphi}: H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是紧的.

必要性.如果$T^n_{\psi_{1}, \psi_{2}, \varphi}: H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是紧的.显然$T^n_{\psi_{1}, \psi_{2}, \varphi}: H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是有界的.设$\{z_{k}\}$${\Bbb D}$中的一个点列使得$|\varphi(z_{k})|\rightarrow1$$(k\rightarrow\infty)$.使用检验函数

注意到$\phi$是正规函数,对$|z|=r<1$,有

可见${f_{k}}$$H(p, q, \phi)$中一个有界的函数列且在${\Bbb D}$的任意紧子集上一致收敛于零.根据引理2.2,可得

由于

利用(3.24)式以及算子$T^n_{\psi_{1}, \psi_{2}, \varphi}: H(p, q, \phi)\rightarrow{\cal Z}_{\mu}$是紧的,我们有

$\begin{equation}\label{qwe42}|C_1(A, B, C, \alpha, n)|\frac{\mu(z_{k})|\psi_1''(z_{k})|\left|\overline{\varphi(z_{k})}\right|^{n}}{\phi(|\varphi(z_k)|)\left(1-\left|\varphi(z_k)\right|^{2}\right)^{1/q+n}}\leq\|T^n_{\psi_{1}, \psi_{2}, \varphi}f_{k}\|_{{\cal Z}_{\mu}}\rightarrow0~ (k\rightarrow\infty).\end{equation}$

利用(3.49)式和$|\varphi(z_{k})|\rightarrow1\ (k\rightarrow\infty)$,得到

因此(3.39)式成立.类似可证(3.40), (3.41)以及(3.42)式成立,此处省去有关细节.

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