单位圆周Lebesgue空间的3阶斜Toeplitz算子的极小约化子空间

Toeplitz算子的约化子空间与不变子空间是近些年算子理论研究的热点，斜Toeplitz算子是Toeplitz算子的自然推广，本文对单位圆周上Lebesgue空间3阶斜Toeplitz算子的约化子空间问题进行研究。通过计算以zN为符号的3阶斜Toeplitz算子在单位圆周上Lebesgue空间的典则基上的作用，对N为模3余1、模3余2及模3余0的3类情形定义了SN，由此得到N的划分，对应给出了Lebesgue空间的一组分解H (N)j。证明对j∈SN，H (N)j均为以zN为符号的3阶斜Toeplitz算子的全部极小约化子空间。推广了关于2阶斜Toeplitz算子约化子空间的相关结果，丰富了Lebesgue空间上斜Toeplitz算子的约化子空间研究，对研究斜Toeplitz算子的结构具有重要意义。     

多复变的解析Besov空间上的Toeplitz算子(英文)

将刻画由复测度μ诱导出的Toeplitz算子Tμ作用在单位球的解析Besov空间上是有界或紧的.对1p∞,α-1,μ是n上的复测度,Toeplitz算子Tαμ作用到Bp上是有界的当且仅当测度|Pα,n+1(μ)(z)|p(1-|z|2)p(n+1-α)dυ(z)是一个(Bp,p)-Carleson测度.在同样的条件下,Toeplitz算子Tμα作用到Bp上是紧的当且仅当测度|Pα,n+1(μ)(z)|p(1-|z|2)p(n+1-α)dυ(z)是一个消失的(Bp,p)-Carleson测度.     

Hardy空间上乘法算子的约化子空间的构造

讨论了Hilbert空间上等距算子的约化子空间问题，并对符号为Blasehke积的Toeplitz算子给出了其约化子空间的具体构造．     

Cn中单位球上加权Bloch空间上的复合算子

对于单复变情形, Bloch空间、小Bloch空间上的复合算子以及加权复合算子的研究已有很多结果.对于Cn中的单位球Bn,通过定义其上的加权Bloch空间Blog={f∈H(Bn):supz∈Bn(1-|z|)ln 2/1-|z| f(z)|< ∞},其中H(Bn)为单位球上全纯函数的全体,f(z)=( f/ z1,…, f/ zn)为f的梯度函数,作者刻画了此空间上的复合算子的有界性和紧性,并得到了充要条件.     

双圆盘上一类解析Toeplitz算子的约化子空间

使用一种新的方法推广了单位圆盘上的解析Toeplitz算子Tx^n的约化子空间问题。     

乘积空间r∏i=1 D上的一类Toeplitz型算子

假设L(→)α.2(r∏i=1 D,dμ(→)α)是乘积空间r∏i=1 D上的带有加权测度dμ(→)α(z)= r∏i=1α+1/π(1-| z|2)ai dm(z)的平方可积函数空间,在本文中我们首先给出了空间L(→)α.2(r∏i=1 D,dμ(→)α)的一个完全正交分解,然后我们定义了一类Toeplitz型算子Tkb,并且证明了它们的有界性、紧性及Schatten-von Neumann性质.     

Fock-Sobolev空间上多重径向符号Toeplitz算子的换位

研究多复变量的Fock-Sobolev空间上多重径向符号Toeplitz算子的换位问题,对φ是以z,z珋为变量的多重径向多项式函数且ψ为多项式有界函数情形,得到了Toeplitz算子T_φ与T_ψ交换的充要条件,还给出了几个有趣的例子和结论.     

对数Bergman 型空间到Bloch空间上的Stevic-Sharma 算子

设D是复平面中的开单位圆盘,φ是D到自身的解析映射,H(D)是D上的解析函数空间.为了统一研究复合算子、乘积算子和微分算子三者的乘积,Stevic和Sharma引进了如下的Stevic-Sharma算子:T_(φ1,φ2),_φf(z)=ψ_1(z)f(φ(z))+ψ_2(z)f′(φ(zf∈H(D),其中ψ_1,ψ_2∈H(D).本文利用符号函数给出了对数Bergman型空间到Bloch空间上Stevic-Sharma算子的有界性、紧性刻画.     

加正规权Bergman空间上的Toeplitz算子

令ω为正规权,对于单位圆盘D上加正规权的Bergman空间A_ω~p(D),其上的投影算子为P_ω。现给定一个正Borel测度μ和一个与ω不同的正规权ν,以μ为符号的且与投影算子P_ω相关的Toeplitz算子为T_μ~ω:Apν(D)→A_ν~q(D)。借助关于正规权的性质、再生核的估算以及Berezin变换得出,当1 相似文献   

加权复合算子是渐近Toeplitz算子

目的 研究Hardy空间上加权复合算子与渐近Toeplitz算子的关系.方法 采用泛函分析和复分析进行研究.结果 主要证明Hardy空间上每一个加权复合算子都是渐近Toeplitz算子.结论 证明了Hardy空间上加权复合算子是渐近Toeplitz算子,在已有文献的相关结果上进行了推广和统一.     

关于一类高阶齐次线性微分方程解的增长性

 研究了高阶线性齐次微分方程
f ^(k)+A_k－1(z)P_k－1(e ^z)f ^′ +…+A₁(z)P₁(e^z)f ^′ +A₀(z)P₀(e^z)f=0
解的增长性,其中A_j(z)≠0(j=0,1,…,k－1)是整函数,P_j(e^z)(j=0,1,…,k－1)是e^z的非常数多项式,它们的常数项都为零,且次数不相等。证明了该微分方程的每一个非零解有无穷级。     

具有极大正规化子的有限群

设群G是有限群.如果对G的任意循环子群A,都存在素数p,使得|G∶N_G(A)||p,那么称G为NP-群.利用循环群的自同构群的性质和群作用等处理手段,证明了有限NP-群G是亚交换群,进而改进了目前已有的关于NP-群已经取得的结论,即有限NP-群G的导长至多是3.     

Average widths and optimal recovery of multivariate Besov classes inL p (Rd)

Some weak asymptotic results for average σ-K width and average σ_L width of the isotropic Besov classes S r pθB(R d), S r pθb(R d) and the anisotropic Besov classes S r pθB(R d), S r pθb(R d) in L p(R d) (1≤p<∞) are obtained, and the corresponding weak asymptotic optimal subspaces are identified. Furthermore, the weak asymptotic behavior of optimal recovery is established for the isotropic Besov classes S r pθB(R d) in L p(R d) (1≤p≤∞).     

The isotopic abundance and atomic weight of natural uranium

Conclusion The published measurement data of atomic weight of uranium are shown in table 4^[9]. The best results are those measured by Smith and Cowanet al. A _r (U) = 238.028 79–238.028 90(3), their result error being ISD. The evaluated value of IUPAC-CAWIA is A_r(U)=238.028 9(1). In this work, the result is A_r(U) = 238.028 91(4). The combined uncertainty has been given according to 2SD of the measurement data through the calibration of a series of standard materials of uranium isotopes. It is reasonable to conclude that in this work the uncertainty which characterizes the measurement quality is better than other published data.     

磁性纳米颗粒系统的铁磁共振和共振线宽分析

 对非相互作用磁性纳米颗粒系统的FMR线型模型进行了研究,以铁磁体从应用场中获得自由能F为例,导出磁性颗粒在较小各向异性时,共振场H_r与有效各向异性场H_A^eff的关系,这个结果与Raikher和Stepanou的结果一致.继而还对共振场线宽进行了分析,并与Smit和Beljers模型进行了比较,其结论说明:在超顺磁区域有效各向异性场H_A^eff对塞曼(Zeeman)相互作用和附加应用场H是不确定的.尤其是这种情况在H_A^eff较小、高温(高温区域),且H_A^eff≈H时,变得更显著.为此提出了随机颗粒阵列及参数特征对这个结果的影响机制.     

An extrapolation theorem on martingale spaces with Ap weights

In this paper, we prove an extrapolation theorem of operators in martingale spaces with A _p weights, which shows that for operators T defined on martingale space L _u ¹ , if T is bounded on martingale space L ^p0(w) for some 1 < p ₀ < ∞ and every, w∈ A _∞, so it is on L ^p,s (w) for every 1 < p, s < ∞, and w ∈ A _∞. We also get some properties of A _p weights and prove that if w ∈ A ₁, then the maximal operator M is bounded on L ^p,q (w) with 1 < p < ∞, 1 < q ≤ ∞.     

关于矩阵方程AXB-C=0的最佳逼近解的一个注记

举反例说明：对于矩阵的2-范数，存在矩阵A，B和C，使得A^†CB^†不是矩阵方程AXB-C=0的最佳逼近解，其中A^†和B^†分别是A和B的Moore-Penrose逆.     

The Distribution of a CP-asymmetric quantity in the decay channel J / Ψ → π + π ? π 0

The distribution of a CP-asymmetric quantityA in the decay channelJ/ψ→π ⁺ π ⁻ π ⁰ is investigated. This dimensionless quantityA is constructed from the momenta of the π-meson final states, namely A=P _x ^{π +} P _y ^{π −} -P _x ^{π −} P _y ^{π −}, whereP _h,P _x ^h andP _y ^h are the module of the momentum of a hadron h, the x- and y-components of that momentum respectively, theJ/ψ particle is produced by e⁺ e⁻ collision, and the direction of the momentum of e⁺ is taken to be the positive direction ofz axis. There would exists the violation under the combined transformation of charge conjugation and space reflection (CP violation) when the average ofA among a lot of events, 〈A〉, be examined to be nonzero clearly from data. In this way, 748 events are selected from the BES experimental data, and analyzed. The corresponding averageA-value is measured to be 〈A〉 = 0.010 39 ± 0.014 61 ± 0.015 2. Further, some discussion of our result, the size of the data sample being need for further attempt and a possible perspective are given.     

Correlation between structure and hardness of magnetron sputtering deposited CNx films

Carbon nitride films are deposited on Si (001) substrates by reactive dc magnetron sputtering graphite in a pure N2 discharge. The structure of carbon nitride films has been probed using Fourier transformation infrared, near edge X-ray absorption fine structure (NEXAFS) and high resolution electron microscopy (HREM), and the hardness has been evaluated in nanoin-dentation experiments. FTIR spectra show that N atoms are bound to sp1, sp2, and sp3 hybridized C atoms. C1s NEXAFS spectra show that the intensity of π* resonance is the lowest for the film grown at substrate temperature TS = 350℃, with a turbostratic-like structure and high hardness, while it is the highest for the film grown at TS = 100℃, with an amorphous structure and low hardness. The correlation between the structure and hardness of carbon nitride films has been discussed.