新题征展(32)

A　题组新编1.对于任意 x∈ R函数 f (x)都满足f(x 2 ) =f (2 - x) .(1)如果方程 f(x) =0恰好有 2 0 0 2个不同实根 ,则这些根之和为 (　 ) .(A) 0　 (B) 2 0 0 2　 (C) 4 0 0 4　 (D) 80 0 8(2 )如果方程 f (x 2 ) =0恰好有 2 0 0 2个不同的实根 ,则这些根之和为 (　 ) .(A) 0　 (B) 2 0 0 2　 (C) 4 0 0 4　 (D) 80 0 8(3)如果方程 f(x - 2 ) =0 ,恰好有 2 0 0 2个不同的实根 ,则这些根之和为 (　 ) .(A) 0　 (B) 2 0 0 2　 (C) 4 0 0 4　 (D) 80 0 8(4)如果方程 f (x 1) =0恰好有 2 0 0 3个不同的实根 ,则这些根之和为 (　 ) .(…     

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.     

微机电系统及其应用

1 引言请想像这样的景像，用微小的机器干各种活。有的使汽车运行更加平稳安全，免除交通事故中千万人遇难。有的则以每秒数拍（1015比特）速率处理信息，从全球网站为人们下载影视节目。另一些能以前所未有的灵敏度和精确度进行科学测量。晶片大小的化工厂则能在需要的时间和地点制造危险的材料。这样的景像现已出现：我们正生活于其中，这就是现代的硅微机械世界[1]。这个世界在40多年前就由Richard Feynman以惊人的先见所预言，当时晶体三极管仍是刚发明而未被验证的技术，集成电路则在多年后才出现。在其1959年的讲话“底层仍有许多空…     

有界域上具有离散全纯核的Koppelman公式与-方程

D是Cn空间中具有逐块C(1)边界的有界域,该文建立了D上一个具有离散局部全纯核的 (0,q)形式的Koppelman积分公式及其相应的■-方程解的积分表示和它的内闭一致估计式.     

第32届国际数学奥林匹克试题及解答

1.(苏联提供)已给△ABC,设I是它的内心,角A,B,C的内角平分线分别与其对边交于A′,B′,C′。求证     

有界域上具有离散全纯核的Koppelman公式与方程

D是C^n空间中具有逐块C(1)边界的有界域，该文建立了D上一个具有离散局部全纯核的(0，q)形式的Koppelman积分公式及其相应的方程解的积分表示和它的内闭一致估计式。     

Wey1代数中的消元法与q恒等式（英）

For the algorithmic proof of q-proper-hypergeometric identities, H.Wilf and D.Zeiberg gave a theoretical frame work. In [1], they proved that q-proper-hypergeometric terms satisfy recurrence relations with polynomial coefficients and could obtain quite explicit bounds for the order of such a recurrence. But how can we find the recurrence relations?We consider single-variable q-proper-hypergeometric identities based on Zeilberg's basic idea. To find the recurrence relations, an elimination in the non-commutative Weyl algebra has been developed. Thereby we obtained the algorithm of proving single-variable q-proper-hypergeometric identities.