$L^{p}_{[0,1]}$空间M\"{u}ntz有理逼近的Jackson型估计 (英)

设$\Lambda=\{\lambda_{n}\}_{n=1}^{\infty}$为正的实数数列, 且当$n\rightarrow\infty$时, 有$\lambda_{n}\searrow 0$.本文给出了当 $\lambda_{n}\leq Mn^{-\frac{1}{2}},\;n=1,2, \cdots ,$(其中$M>0$为一正常数)时M\"{u}ntz系统$\{x^{\lambda_n}\}$的有理函数在$ L_{[0,1]} ^{p}$空间的逼近速度,主要结论为$R_{n} (f, \Lambda )_{L^{p}}\leq C_M \omega (f, n^{-\frac{1}{2}})_{L^{p}},\;1 \leq p \leq \infty.$     

广义线性回归极大似然估计的强相合性

设有该文第1节所描述的广义线性回归模型,以$\underline{\lambda}_n$和$\overline{\lambda}_n$分别记$\sum\limits_{i=1}^{n}Z_iZ_i^{\prime}$的最小和最大特征根,$\hat{\beta}_n$记$\beta_0$的极大似然估计.在文献[1]中,当\{$Z_i,i\ge1$\}有界时得到$\hat{\beta}_n$强相合的充分条件,在自然联系和非自然联系下分别为$\underline{\lambda}_n\rightarrow\infty$, $(\overline{\lambda}_n)^{1/2+\delta}=O(\underline{\lambda}_n)$（对某$\delta>0$)以及$\underline{\lambda}_n\rightarrow\infty$, $\overline{\lambda}_n=O(\underline{\lambda}_n)$.作者将后一结果改进为只要求$(\overline{\lambda}_n)^{1/2+\delta}=O(\underline{\lambda}_n)$,从而与自然联系情况下的条件达到一致.     

一类深度1的可迁模Lie超代数

建立了满足如下条件的可迁$\mathbb{Z}$-分次模Lie超代数$\frak{g}=\oplus_{-1\leq i\leq r}\frak{g}_{i}$的嵌入定理:(i) $\frak{g}_{0}\simeq \widetilde{\mathrm{p}}(\frak{g}_{-1}) $ 并且$\frak{g}_{0}$-模 $\frak{g}_{-1}$ 同构于$\widetilde{\mathrm{p}}(\frak{g}_{-1})$的自然模;(ii) $\dim \frak{g}_1=\frac 23 n(2n^2+1),$ 其中 $n=\frac{1}{2} \dim \frak{g}_{-1}.$特别地, 证明了满足上述条件的有限维单模Lie超代数同构于奇Hamilton模Lie超代数.对局限Lie超代数也做了相应的讨论.     

UNBOUNDED SELF-ADJOINT OPERATOR ΠK SPACE

如果A是Πsubsub空间上的自共轭算子，由文[1]可知存在空间昨一个标准分解 \[{\Pi _k} = N \oplus \{ Z + {Z^*}\} \oplus P\] 在此分解下，A有三角模型\[A = \{ S,{A_N},{A_p},F,G,Q\} \].利用三角模型，我们直接证明了 定理1设A是\[{\Pi _k}\]上的-共轭算子，n是任何自然数，那末\[{A^n}\]也是自共轭算子. 定理2设A是\[{A^n}\]上的自共轭算子，那末对所有的\[{A^n}(n = 1,2,...)\]，存在一个公共 的标准分解，在此分解下 \[\begin{gathered} {A^n} = \{ {S^n},A_N^n,A_P^n,\sum\limits_{i = 0}^{n - 1} {{S^i}} FA_N^{n - 1 - i},\sum\limits_{i = 0}^{n - 1} {{S^i}GA_P^{n - 1 - i}} , \hfill \ \sum\limits_{i = 0}^{n - 1} {{S^i}} Q{S^{*n - 1 - i}} - \sum\limits_{i + j + k = n - 2} {{S^i}(FA_N^j{F^*} + GA_P^j{G^*}){S^{*k}}} \} \hfill \\ \end{gathered} \] 定理3 设A是瓜空间上的自共轭算子，\[\sigma (A) \subset [0,\infty ),0 \notin {\sigma _P}(A),\]，那末存在唯 一的自共轭算子A1，满足\[A_1^n = A,\sigma ({A_1}) \subset [0,\infty )\] 其次，我们研究了谱系在临界点附近的性状.记临界点全体为\[C(A)\]).对 \[{\lambda _0} \in C(A)\]记S与入0相应的最高阶根向量的阶数为\[r({\lambda _0})\] 定理4设A是\[{\Pi _k}\]空间上的无界自共轭算子，\[C(A) \cap ({\mu _1},{\nu _1}) = \{ {\lambda _0}\} \],那末以下四 个命题等价： (i）\[\mathop {sup}\limits_{\mu ,\nu } \{ \left\| {{E_{\mu \nu }}} \right\||{\lambda _0} \in (\mu ,\nu ) \subset ({\mu _1},{\nu _1})\} < \infty \] (ii）\[{\mu ^{{\text{1}}}}...,{\mu ^{{{\text{k}}_{\text{0}}}}}\]是全有限的测度； （iii）\[s - \lim {\kern 1pt} {\kern 1pt} {\kern 1pt} {E_{\mu \nu }}\]存在； （iv)A与\[{\lambda _0}\]相应的根子空间\[{\Phi _{{\lambda _0}}}\]非退化；这里\[{\mu ^{{\text{1}}}}...,{\mu ^{{{\text{k}}_{\text{0}}}}}\]是由\[{A_P}\]与G导出的测度. 定通5 设A是\[{\Pi _k}\]上自共轭算子，\[{\lambda _0} \in C(A),r({\lambda _0}) = n\]，那么 （i）\[{E_{\mu \nu }}\]在\[{{\lambda _0}}\]处的奇性次数不超过2n， （ii）\[s - \mathop {\lim }\limits_{\varepsilon \to 0} \int_{[{M_1},{\lambda _0} - \varepsilon )} {(t - {\lambda _0}} {)^{2n}}d{E_t},s - \mathop {\lim }\limits_{\varepsilon \to 0} \int_{[{\lambda _0} + \varepsilon ,{M_2})} {(t - {\lambda _0}} {)^{2n}}d{E_t},\]存在。这里\[{M_1},{M_2}\]满足\[[{M_1},{M_2}] \cap C(A) = \{ {\lambda _0}\} \] 定理6 设A是\[{\Pi _k}\]上的自共轭算子，临界点集\[C(A) = \{ {\lambda _1},...,{\lambda _l},{\lambda _{l + 1}},{\overline \lambda _{l + 1}},...,{\lambda _{l + p}},{\overline \lambda _{l + p}},\]，这里\[\operatorname{Im} {\lambda _v} = 0(1 \leqslant \nu \leqslant l),r({\lambda _\nu }) = {n_\nu }\]那么有 \[{(\lambda - A)^{ - 1}} = \int_{ - \infty }^\infty {K(\lambda ,t)d{E_t}} + \sum\limits_{\nu = 1}^l {\sum\limits_{i = 1}^{2{n_\nu } + 1} {\frac{{{B_{\nu i}}}}{{{{(\lambda - {\lambda _\nu })}^i}}}} } + \sum\limits_{\nu = l + 1}^{l + p} {\sum\limits_{i = 1}^{{n_\nu }} {[\frac{{{B_{\nu i}}}}{{{{(\lambda - {\lambda _\nu })}^i}}}} } + \frac{{B_{\nu i}^ + }}{{{{(\lambda - {{\overline \lambda }_v})}^i}}}]\] 这里 \[K(\lambda ,t) = \frac{1}{{\lambda - t}} - \sum\limits_{v = 1}^l {\delta (t - {\lambda _v}} )\sum\limits_{i = 1}^{2{n_v}} {\frac{{{{(t - {\lambda _v})}^{i - 1}}}}{{{{(\lambda - {\lambda _v})}^i}}}} ,\delta \lambda {\text{ = }}\left\{ \begin{gathered} {\text{1}}{\text{|}}\lambda {\text{| < }}\delta \hfill \ {\text{0}}{\text{|}}\lambda {\text{|}} \geqslant \delta \hfill \\ \end{gathered} \right.\] \[0 < \delta < \mathop {\min }\limits_\begin{subarray}{l} 1 \leqslant \mu ,v \leqslant l \\ {\lambda _\mu } \ne {\lambda _v} \end{subarray} |{\lambda _\mu } - {\lambda _v}|\].对\[1 \leqslant v \leqslant l\]，\[{B_{vi}}\]是\[{\Pi _k}\]上的有界自共轭算子，而当\[l + 1 \leqslant v \leqslant l + p\]时，\[{B_{vi}} = {({\lambda _\mu } - S)^{i - 1}}{P_{\lambda v}}\]是以与\[{{\lambda _v}}\]相应的根子空间为值域的某些平行投影. 定理7 在定理6的条件下，有 \[\begin{gathered} {\text{f}}(A) = \int_{ - \infty }^\infty {[f(t) - \sum\limits_{v = 1}^l {\delta (t - {\lambda _v}} } )\sum\limits_{i = 0}^{2{n_v} - 1} {\frac{{{f^{(i)}}({\lambda _v})}}{{i!}}} (t - {\lambda _v})d{E_t} \hfill \ {\text{ + }}\sum\limits_{{\text{v = 1}}}^{\text{l}} {\sum\limits_{i = 0}^{2{n_v}} {\frac{{{f^{(i)}}({\lambda _0})}}{{i!}}} } {B_v} + \sum\limits_{v = l + 1}^{l + p} {\sum\limits_{i = 0}^{{n_v} - 1} {[\frac{{{f^{(i)}}({\lambda _v})}}{{i!}}} } {B_{vi}} + \frac{{{f^{(i)}}({{\overline \lambda }_v})}}{{i!}}B_{vi}^ + ] \hfill \\ \end{gathered} \] 这里\[f(\lambda )\]在\[\sigma (A)\]的一个邻域内解析. 为了建立更一般的算子演算，我们引入两个特殊的代数： \[{\Omega _n} = \{ (f,\{ {a_i}\} _{i = 0}^{2n})|f\]为Borel可测函数，\[\{ {a_i}\} \]为一常数}。对\[F = (f,\{ {a_i}\} ) \in {\Omega _n},G = (g,\{ {b_i}\} ) \in {\Omega _n}\]，定义 \[\begin{gathered} \alpha F + \beta G = (\alpha f + \beta G,\{ \alpha {a_i} + \beta {b_i}\} ) \hfill \ F \cdot G = (f \cdot g,\{ \sum\limits_{j = 0}^i {{a_j}} {b_{i - j}}\} ),\overline F = (\overline f ,\{ {\overline a _i}\} ) \hfill \\ \end{gathered} \] 显然\[{\Omega _n}\]是一个交换代数，它的子代数\[{\omega _n}\]定义为 \[{\omega _n} = \{ F = (f,\{ {a_i}\} ) \in {\Omega _n}|\]在0点的一个与F有关的邻域中，成立\[{\text{|f(t) - }}\sum\limits_{i = 0}^{2n} {a{t^i}} | \leqslant {M_F}|t{|^{2n + 1}},{M_F}\]与F有关} 定义 设A是\[{\Pi _k}\]上的自共轭算子，C（A）={0}，r(0)=n,对\[F = (f,\{ {a_i}\} ) \in {\omega _n}\]，定义 \[\begin{gathered} FA{\text{ = }}\int_{{\text{ - }}\infty }^\infty {|f(t) - \sum\limits_{i = 0}^{2n} {{a_i}} } {t^i}{|^2}d{E_t} + \sum\limits_{i = 0}^{2n} {{a_i}} {A^i} \hfill \ DF(A)) = D({A^{2n}}) \cap \{ x \in {\Pi _k}\int_{{\text{ - }}\infty }^\infty {|f(t) - \sum\limits_{i = 0}^{2n} {{a_i}} } {t^i}{|^2}d{\left\| {{E_t}x} \right\|^2} < \infty \hfill \\ \end{gathered} \] 如果f解析，\[F = (f,\{ \frac{{{f^{(i)}}(0)}}{{i!}}\} )\]，那么可得F（A）=f（A）。 定理8 设A是有界自共轭算子，C（A）={0}，r（0）=n，\[G \in {\omega _n}\]，那么 \[\begin{gathered} \overline F (A) = {[F(A)]^ + },(\alpha F + \beta G)(A) = \alpha F(A) + \beta G(A) \hfill \ (FG)(A) = F(A)G(A). \hfill \\ \end{gathered} \] 定理9 设A是\[{\Pi _k}\]上的自共轭算子，C（A）={0}，r（0）=n，\[{F_1} = ({f_1},\{ {a_i}\} ) \in {\Omega _n}\]，\[{F_2} = ({f_2},\{ {a_i}\} ) \in {\omega _n},{f_1},{f_2}\]在\[( - \infty ,\infty )\]连续，在\[\sigma (A)\]上恒等，那么\[{F_1}(A) = {F_2}(A)\]。 定理10 设A是\[{\Pi _k}\]上自共轭算子C（A）={0}，r（0）=n，\[F = (f,\{ {a_i}\} ) \in {\Omega _n}\]f是连续函数，那么\[\sigma (F(A)) = \{ f(t)|t \in \sigma (A)\} \]。 在定理11中，我们建立了F（A）的三角模型并由此证明当\[F = \overline F \]时，\[C(F(A)) = \{ f(t)|t \in C(A)\} \] 定理12 设A施可析\[{\Pi _k}\]空间上的自共轭算子，C（A）={0}，r（0）=n，与0相应的根子空间非退化，T是稠定闭算子，那么\[T \in {\{ A\} ^{'}}\]的充要条件是存在\[F \in {\Omega _n}\]，使T=F（A）。这里\[{\{ A\} ^{'}} = \{ T|\]对满足\[BA \subset AB\]的有界算子B，均有\[BT \subset TB\]}     

在Banach空间中推广的 Roper-Suffridge算子(III)

假定 $X$ 是具有范数$\|\cdot\|$的复 Banach 空间, $n$ 是一个满足 $\dim X\geq n\geq2$的正整数. 本文考虑由下式定义的推广的Roper-Suffridge算子 $\Phi_{n,\beta_2, \gamma_2, \ldots , \beta_{n+1}, \gamma_{n+1}}(f)$: \begin{equation} \begin{array}{lll} \Phi _{n, \beta_2, \gamma_2, \ldots, \beta_{n+1},\gamma_{n+1}}(f)(x) &;\hspace{-3mm}=&;\hspace{-3mm}\dl\he{j=1}{n}\bigg(\frac{f(x^*_1(x))}{x^*_1(x)})\bigg)^{\beta_j}(f''(x^*_1(x))^{\gamma_j}x^*_j(x) x_j\\ &;&;+\bigg(\dl\frac{f(x^*_1(x))}{x^*_1(x)}\bigg)^{\beta_{n+1}}(f''(x^*_1(x)))^{\gamma_{n+1}}\bigg(x-\dl\he{j=1}{n}x^*_j(x) x_j\bigg),\nonumber \end{array} \end{equation} 其中 $x\in\Omega_{p_1, p_2, \ldots, p_{n+1}}$, $\beta_1=1, \gamma_1=0$ 和 \begin{equation} \begin{array}{lll} \Omega_{p_1, p_2, \ldots, p_{n+1}}=\bigg\{x\in X: \dl\he{j=1}{n}| x^*_j(x)|^{p_j}+\bigg\|x-\dl\he{j=1}{n}x^*_j(x)x_j\bigg\|^{p_{n+1}}<1\bigg\},\nonumber \end{array} \end{equation} 这里 $p_j>1 \,( j=1, 2,\ldots, n+1$), 线性无关族 $\{x_1, x_2, \ldots, x_n \}\subset X $ 与 $\{x^*_1, x^*_2, \ldots, x^*_n \}\subset X^* $ 满足 $x^*_j(x_j)=\|x_j\|=1 (j=1, 2, \ldots, n)$ 和 $x^*_j(x_k)=0 \, (j\neq k)$, 我们选取幂函数的单值分支满足 $(\frac{f(\xi)}{\xi})^{\beta_j}|_{\xi=0}= 1$ 和 $(f''(\xi))^{\gamma_j}|_{\xi=0}=1, \, j=2, \ldots , n+1$. 本文将证明: 对某些合适的常数$\beta_j, \gamma_j$, 算子$\Phi_{n,\beta_2, \gamma_2, \ldots, \beta_{n+1}, \gamma_{n+1}}(f)$ 在$\Omega_{p_1, p_2, \ldots , p_{n+1}}$上保持$\alpha$阶的殆$\beta$型螺形映照和 $\alpha$阶的$\beta$型螺形映照.     

混合径角$\lambda$中心有界平均振荡空间的一个特征

在这篇文章中,我们通过Hardy算子交换子$\mathrm{H}_b$与它的对偶算子交换子$\mathrm{H}^*_b$, 其中$b\in {\mathrm{CMOL}^{p_2, \lambda}_{\rm rad}L^{p_1}_{\rm ang}(\mathbb R^n)}$,建立了混合径角$\lambda$中心有界平均振荡空间的一个特征.     

$\beta$阶星象函数和凸象函数的几个充分条件的扩展

本文目的是研究了两个新算子$\mathcal{E}_{\alpha, \lambda}^{\gamma}$和$H_{m}^{l}(\alpha_1)$的星形和凸性的几个充分条件, 分别与定义在单位圆盘的广义Mittag-Leffler函数$E_{\alpha, \lambda}^{\gamma}$和广义超几何函数有关.本文得出的结果与早期的一些已知结果建立联系.     

B -值双随机Dirichlet级数的收敛性

主要研究了B -值双随机Dirichlet级数在不同条件(i) {X_n}服从强大数定律,且0<\mathop{\underline{\lim}}\limits_{n-->\infty}\Big\|\frac{\sum\limits_{i=1}^n EX_i}{n}\Big\|\leq \mathop{\overline{\lim}}\limits_{n\to\infty}\Big\|\frac{\sum\limits_{i=1}^n EX_i}{n}\Big\|<+\infty.(ii) {X_{n}}独立不同分布，且\mathop{\underline{\lim}}\limits_{n-->\infty}E||X_n||>0,\quad \sup\limits_{n\geq 1}E||X_n||^p <+\infty \quad (p >1)等条件下的收敛性,得出了收敛横坐标的简洁公式.     

一类分数阶微分方程多点边值问题解的存在性

本文讨论下面一类分数阶微分方程多点边值问题 $$\align &D^{\alpha}_{0+}u(t) = f(t, u(t),~D^{\alpha-1}_{0+}u(t), D^{\alpha-2}_{0+}u(t), D^{\alpha-3}_{0+}u(t)),~~t\in(0,1), \\&I^{4-\alpha}_{0+}u(0) = 0, ~D^{\alpha-1}_{0+}u(0)=\displaystyle{\sum_{i=1}^{m}}\alpha_{i}D^{\alpha-1}_{0+}u(\xi_{i}),\\&D^{\alpha-2}_{0+}u(1)=\sum\limits_ {j=1}^{n}\beta_{j} D^{\alpha-2}_{0+}u(\eta_{j}),~D^{\alpha-3}_{0+}u(1)-D^{\alpha-3}_{0+}u(0)=D^{\alpha-2}_{0+}u(\frac{1}{2}),\endalign$$其中$3<\alpha \leq 4$是一个实数.通过应用Mawhin重合度理论和构建适当的算子,得到了该边值问题解的存在性结果.     

三角Banach代数的Lie弱顺从性

设$\mathcal {A,\ B}$ 是含单位元的Banach代数, $\mathcal M$ 是一个Banach $\mathcal {A,\ B}$-双模. $\mathcal {T}=\left ( \begin{array}{cc} \mathcal {A} & \mathcal M \\ & \mathcal {B} \\ \end{array} \right )$按照通常矩阵加法和乘法,范数定义为$\|\left( \begin{array}{cc} a & m \\ & b\\ \end{array} \right)\|=\|a\|_{\mathcal A}+\|m\|_{\mathcal M}+\|b\|_{\mathcal B}$,构成三角Banach 代数.如果从$\mathcal T$到其$n$次对偶空间$\mathcal T^{n}$上的Lie导子都是标准的,则称$\mathcal T$是Lie $n$弱顺从的.本文研究了三角Banach代数$\mathcal T$上的Lie $n$弱顺从性,证明了有限维套代数是Lie $n$弱顺从的.     

Boundary Values of Cauchy Transforms in Weighted Spaces of Integrable Distributions

Let $ k \in {\shadN} $ , $ w(x) = (1+x^2)^{1/2} $ , $ V^{\prime} _k = w^{k+1} {\cal D}^{\prime} _{L^1} = \{{ \,f \in {\cal S}^{\prime}{:}\; w^{-k-1}f \in {\cal D}^{\prime} _{L^1}}\} $ . For $ f \in V^{\prime} _k $ , let $ C_{\eta ,k\,}f = C_0(\xi \,f) + z^k C_0(\eta \,f/t^k)$ where $ \xi \in {\cal D} $ , $ 0 \leq \xi (x) \leq 1 $ $ \xi (x) = 1 $ in a neighborhood of the origin, $ \eta = 1 - \xi $ , and $ C_0g(z) = \langle g, \fraca {1}{(2i \pi (\cdot - z))} \rangle $ for $ g \in V^{\,\prime} _0 $ , z = x + iy , y p 0 . Using a decomposition of C 0 in terms of Poisson operators, we prove that $ C_{\eta ,k,y} {:}\; f \,\mapsto\, C_{\eta ,k\,}f(\cdot + iy) $ , y p 0 , is a continuous mapping from $ V^{\,\prime} _k $ into $ w^{k+2} {\cal D}_{L^1}$ , where $ {\cal D}_{L^1} = \{ \varphi \in C^\infty {:}\; D^\alpha \varphi \in L^1\ \forall \alpha \in {\shadN} \} $ . Also, it is shown that for $ f \in V^{\,\prime} _k $ , $ C_{\eta ,k\,}f $ admits the following boundary values in the topology of $ V^{\,\prime} _{k+1} : C^+_{\eta ,k\,}f = \lim _{y \to 0+} C_{\eta ,k\,}f(\cdot + iy) = (1/2) (\,f + i S_{\eta ,k\,}f\,); C^-_{\eta ,k\,}f = \lim _{y \to 0-} C_{\eta ,k\,} f(\cdot + iy)= (1/2) (-f + i S_{\eta ,k\,}f ) $ , where $ S_{\eta ,k} $ is the Hilbert transform of index k introduced in a previous article by the first named author. Additional results are established for distributions in subspaces $ G^{\,\prime} _{\eta ,k} = \{ \,f \in V^{\,\prime} _k {:}S_{\eta ,k\,}f \in V^{\,\prime} _k \} $ , $ k \in {\shadN} $ . Algebraic properties are given too, for products of operators C + , C m , S , for suitable indices and topologies.     

Notes on von Neumann–Jordan and James Constants for Absolute Norms on {\mathbb{R}^2}

Let ${\|\cdot\|_{\psi}}$ be the absolute norm on ${\mathbb{R}^2}$ corresponding to a convex function ${\psi}$ on [0, 1] and ${C_{\text{NJ}}(\|\cdot\|_{\psi})}$ its von Neumann–Jordan constant. It is known that ${\max \{M_1^2, M_2^2\} \leq C_{\text{NJ}}(\| \cdot \|_{\psi}) \leq M_1^2 M_2^2}$ , where ${M_1 = \max_{0 \leq t \leq 1} \psi(t)/ \psi_2(t)}$ , ${M_2 = \max_{0\leq t \leq 1} \psi_2(t)/ \psi(t)}$ and ${\psi_2}$ is the corresponding function to the ? ₂-norm. In this paper, we shall present a necessary and sufficient condition for the above right side inequality to attain equality. A corollary, which is valid for the complex case, will cover a couple of previous results. Similar results for the James constant will be presented.     

EXPONENTIAL STABILITY OF LINEAR SYSTEMS IN BANACH SPACES

In this paper the author proves a new fundamental lemma of Hardy-Lebesgne class $\[{H^2}(\sigma )\]$ and by this lemma obtains some fundamental results of exponential stability of $\[{C_0}\]$-semigroup of bounded linear operators in Banach spaces. Specially, if $\[{\omega _s} = \sup \{ {\mathop{\rm Re}\nolimits} \lambda ;\lambda \in \sigma (A) < 0\} \]$ and $\[\sup \{ \left\| {{{(\lambda - A)}^{ - 1}}} \right\|;{\mathop{\rm Re}\nolimits} \lambda \ge \sigma \} < \infty \]$ , where \[\sigma \in ({\omega _s},0)\]) and A is the infinitesimal generator of a $\[{C_0}\]$-semigroup in a Banach space $X$, then $\[(a)\int_0^\infty {{e^{ - \sigma t}}\left| {f({e^{tA}}x)} \right|} dt < \infty \]$, $\[\forall f \in {X^*},x \in X\]$; (b) there exists $\[M > 0\]$ such that $\[\left\| {{e^{tA}}x} \right\| \le N{e^{\sigma t}}\left\| {Ax} \right\|\]$, $\[\forall x \in D(A)\]$; (c) there exists a Banach space $\[\hat X \supset X\]$ such that $\[\left\| {{e^{tA}}x} \right\|\hat x \le {e^{\sigma t}}\left\| x \right\|\hat x,\forall x \in X.\]$.     

Extremal Functions for Adams Inequalities in Dimension Four

Let $\Omega\subset \mathbb{R}^4$ be a smooth bounded domain, $W_0^{2,2}(\Omega)$ be the usual Sobolev space. For any positive integer $\ell$, $\lambda_{\ell}(\Omega)$ is the $\ell$-th eigenvalue of the bi-Laplacian operator. Define $E_{\ell}=E_{\lambda_1(\Omega)}\oplus E_{\lambda_2(\Omega)}\oplus\cdots\oplus E_{\lambda_{\ell}(\Omega)}$, where $E_{\lambda_i(\Omega)}$ is eigenfunction space associated with $\lambda_i(\Omega)$. $E^{\bot}_{\ell}$ denotes the orthogonal complement of $E_\ell$ in $W_0^{2,2}(\Omega)$. For $0\leq\alpha<\lambda_{\ell+1}(\Omega)$, we define a norm by $\|u\|_{2,\alpha}^{2}=\|\Delta u\|^2_2-\alpha \|u\|^2_2$ for $u\in E^\bot_{\ell}$. In this paper, using the blow-up analysis, we prove the following Adams inequalities$$\sup_{u\in E_{\ell}^{\bot},\,\| u\|_{2,\alpha}\leq 1}\int_{\Omega}e^{32\pi^2u^2}{\rm d}x<+\infty;$$moreover, the above supremum can be attained by a function $u_0\in E_{\ell}^{\bot}\cap C^4(\overline{\Omega})$ with $\|u_0\|_{2,\alpha}=1$. This result extends that of Yang (J. Differential Equations, 2015), and complements that of Lu and Yang (Adv. Math. 2009) and Nguyen (arXiv: 1701.08249, 2017).     

Vilenkin-Like系统的不等式

For bounded Vilenkin-Like system, the inequality is also true：
（∑ k=1 ^∞ kp-2｜f^^（k）｜^p）^1/p ≤ C｜｜f｜｜Hp, 0 〈 p ≤ 2,
where f^^（·） denotes the Vilenkin-Like Fourier coefficient of f and the Hardy space Hp（Gm） is defined by means of maximal functions. As a consequence, we prove the strong convergence theorem for bounded Vilenkin-Like Fourier series, i.e.,
（∑ k=1 ^∞ k^p-2｜｜Skf｜｜p^p）^1/p≤C｜｜f｜｜Hp,0〈p〈1.     

Positive Gegenbauer Polynomial Sums and Applications to Starlike Functions

Let $s_n(f,z):=\sum_{k=0}^{n}a_kz^k$ be the $n$th partial sum of $f(z)=\sum_{k=0}^{\infty{}}a_kz^k$. We show that $\RE s_n(f/z,z)>0$ holds for all $z\in\D,\ n\in\N$, and all starlike functions $f$ of order $\lambda$ iff $\lambda_0\leq\lambda<1$ where $\lambda_0=0.654222...$ is the unique solution $\lambda\in(\frac{1}{2},1)$ of the equation $\int_{0}^{3\pi/2}t^{1-2\lambda}\cos t \,dt=0$. Here $\D$ denotes the unit disk in the complex plane $\C$. This result is the best possible with respect to $\lambda_0$. In particular, it shows that for the Gegenbauer polynomials $C_{n}^{\mu}(x)$ we have $\sum_{k=0}^n C_{k}^{\mu}(x)\cos k \theta>0$ for all $n\in\N,\ x\in[-1,1]$, and $0<\mu\leq\mu_0:=1-\lambda_0=0.345778...$. This result complements an inequality of Brown, Wang, and Wilson (1993) and extends a result of Ruscheweyh and Salinas (2000).     

Hardy-Sobolev类上的Bohr型不等式

Let β 〉 0 and Sβ ：= {z ∈ C ： ｜Imz｜ 〈β} be a strip in the complex plane. For an integer r ≥ 0, let H∞^Г,β denote those real-valued functions f on R, which are analytic in Sβ and satisfy the restriction ｜f^（r）（z）｜ ≤ 1, z ∈ Sβ. For σ 〉 0, denote by Bσ the class of functions f which have spectra in （-2πσ, 2πσ）. And let Bσ^⊥ be the class of functions f which have no spectrum in （-2πσ, 2πσ）. We prove an inequality of Bohr type
‖f‖∞≤π/√λ∧σ^r∑k=0^∞（-1）^k（r＋1）/（2k＋1）^rsinh（（2k＋1）2σβ）,f∈H∞^r,β∩B1/σ,
where λ∈（0,1）,∧and ∧′are the complete elliptic integrals of the first kind for the moduli λ and λ′=√1- λ^2,respectively,and λ satisfies
4∧β/π∧′=1/σ.
The constant in the above inequality is exact.     

Estimates on the mean growth of functions in convex domains of finite type

Let be a bounded convex domain of finite type in with smooth boundary. In this paper, we prove the following inequality:

where , and . This is a generalization of some classical result of Hardy-Littlewood for the case of the unit disc. Using this inequality, we can embed the space into a weighted Bergman space in a convex domain of finite type.

     

Sharp Inequalities for BMO Functions

The purpose of the paper is to study sharp weak-type bounds for functions of bounded mean oscillation. Let 0 p ∞ be a fixed number and let I be an interval contained in R. The author shows that for any φ : I → R and any subset E I of positive measure,For each p, the constant on the right-hand side is the best possible. The proof rests on the explicit evaluation of the associated Bellman function. The result is a complement of the earlier works of Slavin, Vasyunin and Volberg concerning weak-type, L ~p and exponential bounds for the BMO class.     

The Boundedness of Littlewood-Paley Operators with Rough Kernels on Weighted $(L^q,L^p)^{\alpha}(\mathbf{R}^n)$ Spaces

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 $1 < q\leq \alpha < p\leq \infty$.