共查询到17条相似文献,搜索用时 343 毫秒
1.
设$u \in H(D), \ \phi$为$D$上的解析自映射,定义$H(D)$上的加权复合算子为$u C_{\phi}(f)=$$uf\circ\phi$, \ $f\in H(D)$.本文得到了从$A^{p}_{\alpha}$到$A^{\infty}(\varphi)\ (A_{0}^{\infty}(\varphi))$的加权复合算子$u C_{\phi}$的有界性和紧性的充要条件. 相似文献
2.
本文的主要建立非齐性度量测度空间上双线性强奇异积分算子$\widetilde{T}$及交换子$\widetilde{T}_{b_{1},b_{2}}$在广义Morrey空间$M^{u}_{p}(\mu)$上的有界性. 在假设Lebesgue可测函数$u, u_{1}, u_{2}\in\mathbb{W}_{\tau}$, $u_{1}u_{2}=u$,且$\tau\in(0,2)$. 证明了算子$\widetilde{T}$是从乘积空间$M^{u_{1}}_{p_{1}}(\mu)\times M^{u_{2}}_{p_{2}}(\mu)$到空间$M^{u}_{p}(\mu)$有界的, 也是从乘积空间$M^{u_{1}}_{p_{1}}(\mu)\times M^{u_{2}}_{p_{2}}(\mu)$到广义弱Morrey空间$WM^{u}_{p}(\mu)$有界的,其中$\frac{1}{p}=\frac{1}{p_{1}}+\frac{1}{p_{2}}$及$1相似文献
3.
本文首先引入满足如下条件$$-\frac{qzD_{q}f(z)}{f(z)}\prec \varphi (z)$$和$$\frac{-(1-\frac{\alpha }{q})qzD_{q}f(z)+\alpha qzD_{q}[zD_{q}f(z)]}{(1-\frac{\alpha}{q})f(z)-\alpha zD_{q}f(z)}\prec \varphi (z)~(\alpha \in\mathbb{C}\backslash (0,1],\ 0
相似文献
4.
主要研究~$L_{2}(\R^{s})$~中的~Riesz~序列和高维~Riesz~多小波基刻画的问题. 由~Sobolev~空间~$(H^{\mu}(\R^{s}))^{r}~(\mu>0)$~中的紧支集向量细分函数 ~$\varphi=(\varphi^{1},\ldots,\varphi^{r})^{\rm T}$~和~$\tilde{\varphi}=({\tilde\varphi}^{1},\ldots,{\tilde\varphi}^{r})^{\rm T}$~出发, 得到~$L_{2}(\R^{s})$~中的两组~Riesz~多小波基~$\{\psi_{j,k}\}$~和~$\{\tilde{\psi}_{j,k}\}.$~ 在刻画中, 向量函数的方括号积~$[f,g]$~和离散卷积方程组是非常重要的工具. 相似文献
5.
本文研究了单位圆盘上从$L^{\infty}(\mathbb{D})$空间到Bloch型空间 $\mathcal{B}_\alpha$ 一类奇异积分算子$Q_\alpha, \alpha>0$的范数, 该算子可以看成投影算子$P$ 的推广,定义如下$$Q_\alpha f(z)=\alpha \int_{\mathbb{D}}\frac{f(w)}{(1-z\bar{w})^{\alpha+1}}\d A(w),$$ 同时我们也得到了该算子从 $C(\overline{\mathbb{D}})$空间到小Bloch型空间$\mathcal{B}_{\alpha,0}$上的范数. 相似文献
6.
研究了与强奇异Calder\'{o}n-Zygmund算子和加权
Lipschitz函数${\rm Lip}_{\beta_0,\omega}$相关的Toeplitz算子$T_b$的sharp极大函数的点态估计,并证明了Toeplitz算子是从
$L^p(\omega)$到$L^q(\omega^{1-q})$上的有界算子.此外, 建立了与强奇异Calder\'{o}n-Zygmund算子和加权
BMO函数${\rm BMO}_{\omega}$相关的Toeplitz算子$T_b$的sharp极大函数的点态估计,并证明了Toeplitz算子是从
$L^p(\mu)$到$L^q(\nu)$上的有界算子.上述结果包含了相应交换子的有界性. 相似文献
7.
设$\mu$是$[0,1)$上的正规函数,
给出了${\bf C}^{\it n}$中单位球$B$上$\mu$-Bloch空间$\beta_{\mu}$中函数的几种刻画. 证明了下列条件是等价的:
(1) $f\in \beta_{\mu}$; \
(2) $f\in H(B)$且函数$\mu(|z|)(1-|z|^{2})^{\gamma-1}R^{\alpha,\gamma}f(z)$ 在$B$上有界;
(3) $f\in H(B)$ 且函数${\mu(|z|)(1-|z|^{2})^{M_{1}-1}\frac{\partial^{M_{1}} f}{\partial z^{m}}(z)}$ 在$B$上有界, 其中$|m|=M_{1}$;
(4) $f\in H(B)$ 且函数${\mu(|z|)(1-|z|^{2})^{M_{2}-1}R^{(M_{2})}f(z)}$ 在$B$上有界. 相似文献
8.
设$\omega_1,\omega_2$为正规函数, $\varphi$是$B_n$ 上的全纯自映射,$ g\in H(B_n)$ 满足 $g(0)=0$. 对所有的$0
相似文献
9.
设$h(G; x) =h(G)$和$[G]_h$分别表示图$G$的伴随多项式和伴随等价类. 文中给出了$[G]_h$的一个新应用. 利用$[G]_h$, 给出了图$H{\;}(H \cong G)$伴随唯一的充要条件, 其中$H=(\bigcup_{i{\in}A}P_i){\bigcup}(\bigcup_{j{\in}B}U_j)$, $A \subseteq A^{'}=\{1,2,3,5\} \bigcup \{2n|n \in N, n \geq 3\}$, $B \subseteq B^{'} 相似文献
10.
本文主要建立由分数次积分$I_{\gamma}$与函数$b\in\mathrm{Lip}_{\beta}(\mu)$生成的交换子$[b, I_{\gamma}]$在以满足几何双倍与上部双倍条件的非齐度量测度空间为底空间的Morrey空间上紧性的充要条件.在假设控制函数$\lambda$满足逆双倍条件下,证明了交换子$[b,I_{\gamma}]$为从Morrey空间$M^{p}_{q}(\mu)$到$M^{s}_{t}(\mu)$紧性当且仅当$b\in\mathrm{Lip}_{\beta}(\mu)$. 相似文献
11.
在一定条件下,证明了(?)~n中单位球上的加权Bergman空间A~p(φ)上的复合算子C_φ是紧算子的充要条件是当|z|→1~-时(1-|x|~2)/(1-|φ(z)|~2)→0. 相似文献
12.
The Boundedness of Littlewood-Paley Operators with Rough Kernels on Weighted $(L^q,L^p)^{\alpha}(\mathbf{R}^n)$ Spaces 下载免费PDF全文
X. M. Wei & S. P. Tao 《分析论及其应用》2013,29(2):135-148
In this paper, we shall deal with the boundedness of the Littlewood-Paley operators with rough kernel. We prove the boundedness of the Lusin-area integral $\mu_{\Omega,s}$ and Littlewood-Paley functions $\mu_{\Omega}$ and $\mu^{*}_{\lambda}$ on the weighted amalgam spaces $(L^{q}_\omega,L^{p})^{\alpha}(\mathbf{R}^{n})$ as $1 < q\leq \alpha < p\leq \infty$. 相似文献
13.
Let H1, H2 and H3 be infinite dimensional separable complex Hilbert spaces. We denote by M(D,V,F) a 3×3 upper triangular operator matrix acting on Hi +H2+ H3 of theform M(D,E,F)=(A D F 0 B F 0 0 C).For given A ∈ B(H1), B ∈ B(H2) and C ∈ B(H3), the sets ∪D,E,F^σp(M(D,E,F)),∪D,E,F ^σr(M(D,E,F)),∪D,E,F ^σc(M(D,E,F)) and ∪D,E,F σ(M(D,E,F)) are characterized, where D ∈ B(H2,H1), E ∈B(H3, H1), F ∈ B(H3,H2) and σ(·), σp(·), σr(·), σc(·) denote the spectrum, the point spectrum, the residual spectrum and the continuous spectrum, respectively. 相似文献
14.
BERGMAN TYPE OPERATOR ON MIXED NORM SPACES WITH APPLICATIONS 总被引:3,自引:0,他引:3
BERGMANTYPEOPERATORONMIXEDNORMSPACESWITHAPPLICATIONSRENGUANGBINSHIJIHUAIAbstractTheauthorsinvestigatetheconditionsforthebou... 相似文献
15.
The aim of this paper is to establish the necessary and sufficient conditions for the compactness of fractional integral commutator[b,Iγ]which is generated by fractional integral Iγand function b∈Lipβ(μ)on Morrey space over non-homogeneous metric measure space,which satisfies the geometrically doubling and upper doubling conditions in the sense of Hytonen.Under assumption that the dominating functionλsatisfies weak reverse doubling condition,the author proves that the commutator[b,Iγ]is compact from Morrey space Mqp(μ)into Morrey space Mts(μ)if and only if b∈Lipβ(μ). 相似文献
16.
In this paper,we construct a function φ in L2(Cn,d Vα) which is unbounded on any neighborhood of each point in Cnsuch that Tφ is a trace class operator on the SegalBargmann space H2(Cn,d Vα).In addition,we also characterize the Schatten p-class Toeplitz operators with positive measure symbols on H2(Cn,d Vα). 相似文献
17.
Let $G_M$ be either the orthogonal group $O_M$ or the
symplectic group $Sp_M$ over the complex field; in the latter case
the non-negative integer $M$ has to be even. Classically, the
irreducible polynomial representations of the group $G_M$ are
labeled by partitions $\mu=(\mu_{1},\mu_{2},\,\ldots)$
such that $\mu^{\prime}_1+\mu^{\prime}_2\le M$ in the case $G_M=O_M$, or
$2\mu^{\prime}_1\le M$ in the case $G_M=Sp_M$. Here
$\mu^{\prime}=(\mu^{\prime}_{1},\mu^{\prime}_{2},\,\ldots)$ is the partition
conjugate to $\mu$. Let $W_\mu$ be the irreducible polynomial
representation of the group $G_M$ corresponding to $\mu$.
Regard $G_N\times G_M$ as a subgroup of $G_{N+M}$.
Then take any irreducible polynomial representation
$W_\lambda$ of the group $G_{N+M}$.
The vector space
$W_{\lambda}(\mu)={\rm Hom}_{\,G_M}( W_\mu, W_\lambda)$
comes with a natural action of the group $G_N$.
Put $n=\lambda_1-\mu_1+\lambda_2-\mu_2+\ldots\,$.
In this article, for any standard Young tableau $\varOmega$ of
skew shape $\lm$ we give a realization of $W_{\lambda}(\mu)$
as a subspace in the $n$-fold tensor product
$(\mathbb{C}^N)^{\bigotimes n}$, compatible with the action of the group $G_N$.
This subspace is determined as the image of a certain linear operator
$F_\varOmega (M)$ on $(\mathbb{C}^N)^{\bigotimes n}$, given by an explicit formula.
When $M=0$ and $W_{\lambda}(\mu)=W_\lambda$ is an irreducible representation of
the group $G_N$, we recover the classical realization of $W_\lambda$
as a subspace in the space of all traceless tensors in $(\mathbb{C}^N)^{\bigotimes n}$.
Then the operator $F_\varOmega\(0)$ may be regarded as the analogue
for $G_N$ of the Young symmetrizer, corresponding to the
standard tableau $\varOmega$ of shape $\lambda$.
This symmetrizer is a certain linear operator on
$\CNn$$(\mathbb{C}^N)^{\bigotimes n} $ with the image equivalent to the irreducible
polynomial representation of the complex general linear group
$GL_N$, corresponding to the partition $\lambda$. Even in the case
$M=0$, our formula for the operator $F_\varOmega(M)$ is new.
Our results are applications of the representation
theory of the twisted Yangian, corresponding to the
subgroup $G_N$ of $GL_N$. This twisted Yangian
is a certain one-sided coideal subalgebra of the Yangian corresponding
to $GL_N$. In particular, $F_\varOmega(M)$ is an intertwining
operator between certain representations of the twisted Yangian
in $(\mathbb{C}^N)^{\bigotimes n}$. 相似文献