插值Blaschke积的两个刻划定理

信据Ｂｌａｓｃｈｋｅ积在Ｈ＾∞的极大理想空间Ｍ上的零点分布，给出了Ｂｌａｓｃｈｋｅ积是插值Ｂｌａｓｃｈｋｅ积的两个刻划定理。     

关于仿射完备极大曲面的一个结果

x：M→A^n 1是一个局部严格凸的超曲面，由定义在一个凸域Ω包含于A^n的严格凸的函数xn 1=f(x1,…,xn)给出，作者引入Blaschke度量G=ρ∑(a^2f/axiaxj)dxidxj,ρ=[det(a^2f/axiaxj)]^-1/(n 2)，并讨论了关于度量G完备的仿射极大曲面的性质．     

整函数在Bergman空间中的逼近

本文给出了在Bergman空间中函数被多项式逼近的阶与被逼近函数是ρ级σ型整函数的充要条件。     

Blaschke积的系数

本文研究了Blaschke积族β_c-{B(Z)-∏((r_k-Z)/(1-r_kZ)) from k=1 to m}的系数,并得到了一些结果。     

Reception and discovery: the nature of Johann Wilhelm Ritter’s invisible rays

Ultraviolet radiation is generally considered to have been discovered by Johann Wilhelm Ritter in 1801. In this article, we study the reception of Ritter’s experiment during the first decade after the event—Ritter’s remaining lifetime. Drawing on the attributional model of discovery, we are interested in whether the German physicists and chemists granted Ritter’s observation the status of a discovery and, if so, of what. Two things are remarkable concerning the early reception, and both have to do more with neglect than with (positive) reception. Firstly, Ritter’s observation was sometimes accepted as a fact but, with the exception of C. J. B. Karsten’s theory of invisible light, it played almost no role in the lively debate about the nature of heat and light. We argue that it was the prevalent discourse based on the metaphysics of Stoffe that prevented a broader reception of Ritter’s invisible rays, not the fact that Ritter himself made his findings a part of his Naturphilosophie. Secondly, with the exception of C. E. Wünsch’s experiments on the visual spectrum, there was no experimental examination of the experiment. We argue that theorizing about ontological systems was more common than experimenting, because, given its social and institutional situation, this was the appropriate way of contributing to physics. Consequently, it was less clear in 1810 than in 1801 what, if anything, had been discovered by Ritter.     

Bergman空间上乘子的酉等价性

在这篇文章中，我们证明了：如果ψ1ψ2……ψ1∈，H∞（D），并且存在某个α∈D，使得（f-f（α））的内函数部分是一个有限的Blaschke乘积，Mψ1，Mψ2…Mψn与Mf作为Bergman空间上的乘子，则的充分必要条件是ψ1＝ψ2＝…＝ψn＝f＝常数，这里n≥2。     

仿射空间中的抛物型螺旋面

螺旋面是由一条平面曲线绕固定轴旋转的同时，沿轴的方向作匀速平移产生的曲面.由于旋转轴类型的不同，螺旋面可以分为椭圆型、双曲型和抛物型三种情况.在三维仿射空间中，利用Blaschke度量研究抛物型螺旋面，并对高斯曲率为零和平均曲率为零的抛物型螺旋面分别进行了分类.当符距h=0时，螺旋运动退化为旋转运动，在此情况下，进一步分类了平坦和极小的抛物型旋转曲面，并得出此时抛物型旋转曲面所满足的方程，最后画出其相应的图像.     

L_p混合质心体均质积分和对偶均质积分Brunn-Minkowski不等式（英文）

定义了新几何体Γ-p,iK和Lp混合调和Blaschke加K＋¨pL的概念,建立了Lp混合质心体Γp,iK的均质积分和对偶均质积分的Brunn-Minkowski不等式,并研究了算子Γp,i和Γ-p,i的单调性.     

圆盘自同构迭代的零点序列与Blaschke乘积

考虑单位圆盘上解析自同构零点的性质,通过计算证明:解析自同构中双曲型的和抛物型的在迭代后得到的零点所生成的Blaschke乘积具有插值性和单分支性,椭圆型的在迭代后得到的零点不趋于边界,不能生成Blaschke乘积.     

非负里奇曲率的完备极值射影Blaschke流形

本文在里奇曲率非负的假定下,解决了李-赵关于极值射影Blaschke流形的一个猜想,得到:若M为非负里奇曲率的n维完备极值射影Blaschke流形,则M等距于En/Γ,其中Γ为自由、纯不连续作用在M上的等距离散子群,M～为M的万有覆盖流形.