A Novel Heat-resisting Surfactant for the Modification of Alumina Nanoparticles

An casy preparation of controlled alumina nanoparticles by the solution precipitate method has been carried out using dendrimer as surfactant.The effects of the amount and size of surfactant on morphological control of powder have also been discussed.     

Highly Selective Diphoshinoamine/Cr(III) Catalysts for Ethylene Tetramerization

Ethylene trimerization has been attracted much attention because of their high selectivity towards 1-hexene1-6. The common belief is that ethylene tetramerization is improbable. This is because if ethylene tetramerization proceeds via the same mechanism o…     

纤维复合媒质中的超声衰减

为了精确估计纤维复合煤质中散射所引起的超声衰减，必须计及纤维之间的多次散射现象本文提出了纤维复合煤质中任一点有效入射声场的计算方法当超声纵波传播方向与纤维轴线相垂直时，散射横波并不影响有效入射声场；导出了考虑多次散射后超声衰减系数的表达式；数值计算了玻璃／金属铝复合媒质中纵波衰减系数随频率的变化关系 关键词：     

一类二元对策问题

讨论一类二元对策问题.在对策双方能力不同的情况下,推导对策双方获胜的充要条件和获胜方获胜的具体对策方案.文后的应用实例说明,本文所讨论的问题具有一定的应用价值.     

FORMATION AND MAGNETIC PROPERTIES OF A NOVEL Gd3(Fe,Ti)29Ny NITRIDE

The novel Gd₃(Fe_0.978Ti_0.022)₂₉ compounds and their nitride have been synthesized. The X-ray diffraction patterns of the Gd₃(Fe,Ti)₂₉N_y and its parent compounds were indexed in the Nd₃(Fe,Ti)₂₉-type structure with a monoclinic symmetry and space group P2₁/c, Both the nitride and the parent compounds exhibit ferrimagnetlc coupling. Nitrogenatio led to an increase in Curie temperature and saturation magnetization. The Curie temperatures are 517K for the parent and 765K for the nitride. The saturation magnetizations σ_s at 4.2K are 101.9A·m²/kg for the parent and 128A·m²/kg for the nitride. Both the nitride and parent exhibit a planar anisotropy. Nitrogenation led to a decrease of the contribution of Fe-sublattice to planar anisotropy. The anisotropy fields at 4.2K are 9.8T for the parent and 6.5 T for the nitride.     

STUDIES ON THE DYNAMICS OF OPTICAL BISTABILITY SWITCHING IN THE INTERNAL FABRY-PEROT CAVITY WITH A CdSxSe1-x-DOPED GLASS CHANNEL WAVEGUIDE

We report the optical bistability in CdS_xSe_1-x-doped glass channel waveguide with rise and fall times of about 24 and 30ps, respectively, in bistable switching by means of fiber coupling input with a power of about 3mW. The third-order nonlinear susceptibility (x⁽³⁾) of CdS_xSe_1-x-doped glass is estimated experimentally to be 1.8×10^-9 esu. The high speed switching and the value of x⁽¹⁾ show that the optical bistability is caused by an optical nonlinearity which can be attributed to the band-filling effect.     

求最小权无三角形完美2-匹配的 O(|V|~3)算法

设 G=(V,E)是一简单图.E(G)和 V(G)分别表示 G 的边集合和顶点集合.G 的一个无三角形2-匹配是一个整数向量 x=(x_e:e∈E(G)),使得x_e≥0,(?)_e∈E(G),(1)x(δ(v))≤2,(?)_v∈V(G),(2)x(γ(s))≤2,(?)S(?)V(G),|S|=3.(3)若 x 进一步使(2)都以等式成立,则 x 称为是无三角形完美2-匹配.文献[1]证明了:(1)—(3)的可行解集合就是 G 的无三角形2-匹配的凸包多面体.[1]还同时给出了求最     

层子模型里介子的分类

在前一工作中我们应用层子模型基本上解释了所有已观察到的较肯定的稳定和不稳定的介子,指出这些介子都可看作是一对层子和反层子在赝标型简谐振子位阶中J~P=0~-和1~-的态以及这两个态的轨道角动量l=1和2的激发态。在这篇短文中,我们将较详细的给出这个结论在实验上的主要依据。     

层子模型里介子的波函数和能级

本文利用Bethe-Salpeter型的方程处理了层子模型中的介子内部波函数,指出如果层子和反层子之间的作用可以用一个赝标型位阱来代表,那么0^-和1^-介子将满足相同的近似迳向波动方程,从而导致SU₆对称性。我们以前曾经证明赝标型位阱是唯一可以导致这个对称性的单一型位阱。我们的位阱是V=V₀+V₁,V₀代表一个超强的深位阱,它的作用是降低层子的原始质量M,使它的有效值M′变得很小,使得层子在强子内部的运动是相对论的。V₁代表数量级为1/M的简谐振子位阱,另外还引入一个张量力来解释自旋和轨道角动量相同态的能级分裂。我们得出基态和角动量激发态0^-和1^-介子的解,基本上解释了所有观察到的介子。我们的理论可以同样处理重子态,只要唯象位阱V₀只有介子的值的一半。     

Λ和∑粒子衰变的上下不对称性

本文计算结果指出,当强作用的影响被考虑以后,超子衰变的上下不对称的实验结果是可以解释的。对衰变的分析可以给出关于强作用的重正化和强度的重要知识。我们的结果指出强作用满足“强作用近似”的条件。