齐次群上的平均振荡问题

本文通过构造ｋ－容许覆盖，定义了齐次群上平均振荡空间，并得到该函数空间上的若干等价范数刻划，拓广了文［４］中的结果。     

二阶非线性摄动常微方程解的振荡性

本文研究下述二阶非线性摄动微分方程（a（t）φ（x（t））x’（t））’＋Q（t，x（t））＝P（t，x（t），X’（t）①的解之振荡性，并得到了振荡定理。     

桥头跳车产生的机理与工程设计对策

桥头跳车在我国道路上已成为通病,对道路服务性和安全行车形成危害。针对道路桥头跳车产生的机理,本文提出了解决的对策。     

关于多线性振荡奇异积分在加权Hardy-型空间上的一致估计

本文对一类具有光滑位相函数的多线性振荡奇异积分算子建立了一致的加权（H^1(R^n),L^1(R^n))估计及一致的加权（HKp(R^n),Kp(R^n)估计。     

液体导热机理与液体导热率方程

本文提出了气体不平衡状态方程,将其移植应用于液体,并导出正常液体导热率方程.经过不同结构类型的110种无机与有机纯质的608个实验值的验证,平均误差为1.75％.显著优于已有方程.     

压型钢板在建筑工程中的应用

通过剖析压型钢板的物理构造，讨论了它的抗腐蚀机理，阐述了压型钢板在建筑工程中的应用现状、应用范围及其在不同应用中需要注意的一些技术问题，介绍了压型钢板的一些安装新技术，并对压型钢板的应用前景进行了展望。     

Entangling Two Multi-atomic Clusters Through a Cavity Field

Two atomic clusters, which have NA and Ns two-level atoms, respectively, are placed in a cavity but separated spatially. There is no direct interaction between the atoms. All the atoms interact with a single-mode of the cavity field. Quantum entanglement between the two atomic clusters is investigated for various initial states of the two atomic clusters and the field. When the cavity field is initially in a Fock state, we find that the time evolution of entanglement quasi-periodically oscillates regardless of the initial states of atoms. The oscillation period increases as the initial photon number increases. When all the atoms in both of the atomic clusters are initially in the excited state, we show that there is no entanglement between the atomic clusters with NA = NB = 1 regardless the initial state of the cavity field. However, when either NA or NB is larger than one, we find that the entanglement always exists even for a strong thermal field. In cases with different initial states of the atomic clusters, we notice that the entanglement becomes stronger as number of the atoms increases. When all the atoms in both of the clusters in the ground state, we also find that the entanglement can be enhanced even by a thermal field. We also notice that a single qubit can be entangled with multi-atoms which are initially in the ground state by the cavity field initially being in vacuum, thermal, coherent, and squeezed states.     

一类非线性常微分方程振荡解的渐近表示

在本文中,我们讨论了非线性常微分方程y"=a0|x|αy3 a1|x|βy2 α2|x|γy α3|x|δ振荡解的渐近表示．在这个方程中将α0,α,α1,β,α2,γ,α3,δ分别换成0,0,6,0,0,0,sgn(x),1就是著名的第一类Painleve方程,而将α0,α,α1,β,α2,γ,α3,δ分别换成2,0,0,0,sgn(x),1,α0,就是著名的第二类Painleve方程．当α0,α,α1,β,α2,γ,α3,δ分别换成-β/3γ,0,0,0,1/γ,1,α,0时,可用于组合KdV方程孤立子解的化简．