The Geometric Construction of WZW Effective Action in Noncommutative Manifold

By constructing close-one-cochain density Ω^12n in the gauge group space we get the Wess-Zumino-Witten (WZW) effective Lagrangian on high-dimensional noncommutative space.Especially consistent anomalies derived from this WZW effective action in noncommutative four-dimensional space coincide with those obtained by L.Bonora etc.(het-th/0002210).     

聚类分析在髁突骨密度分析中的应用

本研究应用聚类分析的方法，对人离休髁突×片进行数字图像技术处理所获得的影像密度数值做了详细分析，取得人髁突不同区的骨密度分布及不同年龄阶段髁突密度变化的情况。该方法避免了人为因素的影响，其结果较客观地反映了髁突的骨质密度；为研究病理状态时髁突骨密度的改变提供参考。     

线性规划问题的矩阵求解方法

单纯形法是求解线性规划问题的基本方法。它的解题思路是,先求一个可行解,经过检验如果不是最优解,则从这个可行解转换到另一个可行解。若后者仍不是最优解,再重复上述     

薄膜阻尼结构的处理位置优化

本文介绍薄膜阻尼结构在使用时，如何选取处理位置才能达到预期的效果．     

D—AKNS族的换位表示

本文根据曹策问教授的想法,求得了与D-AKNS族发展方程相联系的特征值之泛函梯度与Lenard算子对;并由此得到了D-AKNS族非线性发展方程的换位表示。文末还讨论了换位表示与定态D-AKNS方程之间的关系.     

化工传热过程计算方法的分析

通过分析比较化工传热过程计算中的平均温度差法(MTD法)和传热单元数法(NTU法),找出了它们之间的内在联系,结合这两种方法的优点,组合成了一种新的计算方法,应用于化工传热过程的计算,可使计算过程大为简便,同时又可评价换热设备流动型式的合理性。     

一类半参数回归模型的估计理论

考虑半参数回归模型Y=X’β+g(T)+e,其中(X,T)为取值于R^p×[0,1]上的随机向量,β为p×1未知参数向量,g为定义于[0,1]上的未知函数,e为随机误差,Ee=0,Ee²=σ²>0,且(X,T)与e独立。本文综合最近邻和最小二乘的方法定义了β,g和σ²的估计量,g_n^*和。在适当条件下证明了和的渐近正态性,并得到了g_n^*的最优收敛速度。     

条形装箱问题的优化模型和增广Lagrange算法

This paper formulates a two-dimensional strip packing problem as a non-linear programming(NLP)problem and establishes the first-order optimality con-ditions for the NLP problem.A numerical algorithm for solving this NLP problemis given to find exact solutions to strip-packing problems involving up to 10 items.Approximate solutions can be found for big-sized problems by decomposing the setof items into small-sized blocks of which each block adopts the proposed numericalalgorithm.Numerical results show that the approximate solutions to big-sized prob-lems obtained by this method are superior to those by NFDH,FFDH and BFDHapproaches.     

Teleportation of an Arbitrary Multipartite GHZ-Class State by One EPR Pair

We present a scheme for perfectly teleporting an arbitrary and unknown N-particle GHZ-class state from a sender to a receiver. We just need one quantum channel composed of two or three particles in the maximally entangled state. The sender performs one Bell-state measurement on two of her particles and N - 1 Hadamard operations and N - 1 yon Neumann measurements on the rest N - 1 particles. The receiver adopts one corresponding unitary transformation on his particles shared with the sender. After that, the receiver can obtain the original N-particle GHZ-class state by introducing N - 1 ancillary particles and carrying out N - 1 controlled-NOT operations. We also generalize the scheme to the case of controlled teleportation.