Efficient Quantum Cryptography Network without Entanglement and Quantum Memory

An efficient quantum cryptography network protocol is proposed with d-dimensional polarized photons, without resorting to entanglement and quantum memory. A server on the network, say Alice, provides the service for preparing and measuring single photons whose initial state are ｜0〉. The users code the information on the single photons with some unitary operations. To prevent the untrustworthy server Alice from eavesdropping the quantum lines, a nonorthogonal-coding technique is used in the process that the quantum signal is transmitted between the users. This protocol does not require the servers and the users to store the quantum states and almost all of the single photons can be used for carrying the information, which makes it more convenient for application than others with present technology. We also discuss the case with a faint laser pulse.     

Multiparty Quantum Secret Report

A multiparty quantum secret report scheme is proposed with quantum encryption. The boss Alice and her M agents first share a sequence of （M ＋ 1）-particle Greenberger-Horne-Zeilinger （GHZ） states that only Alice knows which state each （M ＋ 1）-particle quantum system is in. Each agent exploits a controlled-not （CNot） gate to encrypt the travelling particle by using the particle in the GHZ state as the control qubit. The boss Alice decrypts the travelling particle with a CNot gate after performing a aσ∞ operation on her particle in the GHZ state or not. After the GHZ states （the quantum key） are used up, the parties check whether there is a vicious eavesdropper, say Eve, monitoring the quantum line, by picking out some samples from the GHZ states shared and measuring them with two measuring bases. After confirming the security of the quantum key, they use the remaining GHZ states repeatedly for the next round of quantum communication. This scheme has the advantage of high intrinsic efficiency for the qubits and total efficiency.     

MoxGe1-x,MoxSi1-x薄膜的非晶形成成份及超导转变温度

用直流吸气溅射法在液氮冷底板上分别制备了Mo_xGe_1-x,Mo_xSi_1-x的薄膜。其形成非晶的成份分别为Ge>22at%,Si>18at％。超导转变临界温度T_c在非晶状态下随着Ge,Si的含量增加而下降(约6—3K)。非晶Mo₇₇Ge₂₃膜的晶化温度为780℃,而非晶Mo₇₈Si₂₂膜的晶化温度为480℃。 关键词：     

硅甲烷CARS光谱的研究

测量和分析了硅甲烷(SiH_4)v_1带和v_3带的CARS光谱,并采用偏振CARS技术,解除了v_1带的影响,获得了完全的v_3带的CARS谱.偏振测量和理论模拟计算给出了v_1带和v_3带Q支峰值间的频率位移及两者喇曼跃迁截面平方的比值.     

光学活性α-松油醇的合成新方法

本文报导在季铵盐存在下用氢型丝光沸石催化α-蒎烯的水合反应,该反应立体选择性地一步合成了光学活性α-松油醇。作者认为主产物α-松油醇的生成是通过离子对协助碳正离子重排进行的。     

分子筛催化萜烯烷氧基化反应的研究 Ⅰ.异菠基烷基醚的合成

本文报导沸石分子筛催化蔌烯(1)、三环烯(2)与C_1～C_4醇发生烷氧基化反应,生成异菠基烷基醚(3a-3g)和副产物6,7,7-三甲基-2-烷氧基双环(2,2,1)庚烷(4a-4g)的结果。产物的结构经红外、质谱、核磁和元素分析测定,此法被认为是一种合成异菠基烷基醚的新方法。文中还讨论了可能的反应机理。     

光学材料中横向SBS的稳态分析

 从非线性光学的耦合波理论出发，建立了种子光入射的窄带泵浦的横向受激布里渊散射的二维理论模型，并对稳态情形进行了数值模拟，得到了散射光强的二维分布。计算表明，散射光场在入射面内呈现出“局部集中”的特点，而且由于“空间压缩”效应，使得获得的最大散射光强远大于初始泵浦光强。还分析了光场及材料参数对获得的散射光强的影响，得出：入射的激光功率密度越大，光学元件的横向尺寸越长，材料的吸收系数越小，受激散射产生的散射光和弹性声波强度就越大，在材料内部引起的应力也越强，从而越有可能造成材料的破坏。     

仲钨酸盐A柱撑化合物Mg12Al6(OH)36(W7O24)·4H2O的合成及其光催化性能研究

光催化降解水中有机污染物并使之矿化为无机物的技术正在引起众多学者的关注[1～3]. 目前, 两类主要的光催化剂为半导体金属氧簇和多金属氧酸盐簇(POM). 然而, 这两类催化剂在使用过程中都存在着催化剂难以回收的缺点. 将POM嵌入层柱双氢氧化物(LDH)中制备POM柱撑化合物是固载POM的有效途径之一[4]. 均相体系中仲钨酸盐A(W7O6-24)的光化学活性已有研究, 它可使22种卤代烃完全降解和矿化[5]. 本文通过阴离子交换反应制备了水不溶性的仲钨酸盐A柱撑化合物Mg12Al6(OH)36(W7O24)*4H2O(缩为Mg2Al-W7), 所用前躯体为Mg4Al2(OH)12TA*xH2O (简写为Mg2Al-TA, TA2-= 对苯二甲酸根离子). Mg2Al-W7在非均相体系中的光化学行为通过水溶液中有机氯杀虫剂六六六(C6H6Cl6, 用HCH表示)的降解与矿化进行了研究. 据报道, 由于六六六非常稳定和难于降解, 目前农田中仍存在数以千吨计的残留的六六六, 国外文献近期仍在报道TiO2光催化降解六六六的方法[6,7]. 我们的研究表明, Mg2Al-W7对降解及矿化六六六有活性, 且催化剂易于分离回收, 并可用于再循环. 这些特点为Mg2Al-W7光催化降解水中其它有机污染物的研究与应用奠定了基础.     

Controlled Remote Preparing of an Arbitrary 2-Qudit State with Two-Particle Entanglements and Positive Operator-Valued Measure

We present a scheme for symmetric controlled remote preparation of an arbitrary 2-qudit state form a sender to either of the two receivers via positive operator-valued measurement and pure entangled two-particle states. The first sender transforms the quantum channel shared by all the agents via POVM according to her knowledge of prepared state. All the senders perform singIe- or two-particle projective measurements on their entangled particles and the receiver can probabilisticaly reconstruct the original state on her entangled particles via unitary transformation and auxiliary qubit. The scheme is optimal as the probability which the receiver prepares the original state equals to the entanglement of the quantum channel. Moreover, it is more convenience in application than others as it requires only two-particle entanglements for preparing an arbitrary two-qudit state.