在单模真空场中利用纠缠GHZ态制备纠缠W态

提出在单模真空场中利用纠缠GHZ态制备纠缠W态方案.3个原子(1,2,3)之间初始为纠缠GHZ态,原子1远离单模真空场,而原子2和原子3进入单模真空场与场相互作用.在原子间耦合量适当时,通过控制单模真空场与原子2和原子3的相互作用时间,对原子1的状态进行测量,制备出理想纠缠W态.     

利用纠缠交换制备最大纠缠态

基于腔QED技术提出利用纠缠交换制备光子-光子和原子-光子最大纠缠态的简便方案.在制备光子-光子最大纠缠态方案中,腔只是被虚拟激发,原子和腔之间没有信息转换,大大降低了对腔品质的要求.在利用双光子共振相互作用制备原子-光子最大纠缠态方案中,只要对单原子的态进行测量,而不需要联合Bell基测量.     

基于重复使用纠缠W态的量子秘密分享

提出了重复使用纠缠W态的量子秘密分享方案.在该方案中,发送方和接受方之间的纠缠W态作为载体,发送方将数据比特与这一载体产生纠缠,再由接受方解除纠缠而最终获得秘密消息.所有这些都由一些简单逻辑门来完成.研究结果表明,窃取或联手欺骗成功的可能性都非常小.     

量子隐形传态中纠缠态制备的研究进展

量子隐形传态是量子力学和信息科学等形成的交叉课题,同时也是近些年来人们研究的热点之一。文章首先回顾了Bennett等人所提出的量子隐形传态的基本思想和基本原理,然后着重介绍了量子隐形传态中的重要步骤,即量子纠缠态的制备及其在传统上和近年来的一些具有代表性的实验实现方案。     

量子纠缠态及可分离态判据

由信息熵理论结合量子力学态矢的特性，提出独立态矢的概念，给出了多粒子量子位纯态纠缠的新定义，指出量子纠缠态实质上是独立态矢的叠加，并进一步给出自旋为1／2的二、四量子位体系纯态的非纠缠态判据。其计算方法简单，物理意义明确。     

多个囚禁离子纠缠态的制备

提出了一个制备任意多个囚禁离子叠加运动相干态的方案.制备的叠加运动相干态在位相空间呈一直线分布,该方案能用来制备任意多个囚禁离子的最大纠缠GHZ态.方案中仅使用了一束驻波光,驻波光的载波频率使得离子发生跃迁,而所有离子同时所处的位置可以不限于激光的波腹而处在任意位置.这能给实验带来许多便利,同时,只要选择激光的Rabi频率足够大,相应的操作时间可以足够短.     

一种类型的三量子比特纠缠态远程制备

提出一种类型三量子比特GHZ态远程制备(RSP)实现方案,利用两量子比特的最大纠缠态(即Bell态)作为量子信道,制备成功几率和经典信息消耗都被一一计算出来.就一般情况来说,根据Alice的测量结果,Bob以1/4的几率能够成功实现GHZ态的远程制备.但是,对于三类特殊态,经额外消耗经典信息后其成功几率能够大大提高至1.0.即此方案是决定性的.     

四粒子纠缠W态的概率隐形传输

提出利用2个二粒子部分纠缠态作为量子信道,实现四粒子纠缠W态的概率隐形传输方案.发送者做3次幺正变换和2次Bell基测量,然后接收者通过引入辅助粒子并做适当的幺正变换,就能以一定的概率完成四粒子纠缠W态的隐形传输.     

MG模型中纠缠态演化的研究

纠缠态是量子通信和量子计算的重要资源。讨论了量子纠缠态在Majumdar-Ghost自旋系统中的演化,纠缠态通过concurrence度量。数值计算结果表明纠缠度与系统耦合系数和演化时间相关。通过选择合适的系统演化时间、耦合系数,在自旋MG系统中可以实现高品质的量子纠缠态制备。     

基于团簇态信道的双粒子纠缠态可控量子隐形传态

提出利用四粒子团簇态传送一个未知两粒子纠缠态从而实现可控量子隐形传态的方案,发送者对她自己拥有的3个粒子做一次三粒子纠缠完备基联合测量,控制者对其拥有的粒子作局域测量,接收者在控制者的帮助下对其自己拥有的两粒子做相应的幺正变换,即可重新构造出发送者要传送的未知态,完成了可控量子隐形传态.     

无粒子损失的W态融合研究综述

纠缠W态是量子通信的关键资源,而融合技术已被证明是制备大规模纠缠W态的有效方法.简要综述几类重要的有粒子损失的W态融合方案及相互关系,并着重阐述无粒子损失的W态融合方案及其物理原理,最后给出总结与展望.     

L1-范数子空间技术的鲁棒建模综述

子空间学习可以通过多种技术来开展,对一些流行且被广泛使用的子空间学习方法,简要回顾其基于L1-范数的鲁棒建模.从主成分分析开始介绍子空间学习技术、线性判别分析以及更一般的图嵌入框架.作为L1-范数的综合利用,进一步讨论具有稀疏性的鲁棒建模.此外,还论述一些应用在神经科学中的相关子空间学习技术.最后,针对基于L1-范数的子空间学习的求解问题,介绍一个有力工具,即边界优化技术.     

利用腔的输入输出过程制备多原子纠缠态(英文)

论文提出一些制备多原子纠缠态的物理方案,这些方案是依靠辅助腔和单光子脉冲相互作用来完成的.即使原子不在Lamb-Dicke体系中,通过此方案产生的纠缠态仍具有很高的保真度.从实验的观点来看,较少的操作数目和简单的装置使此方案更容易实现.     

Atomic homodyne detection of continuous-variable entangled twin-atom states

Historically, the completeness of quantum theory has been questioned using the concept of bipartite continuous-variable entanglement. The non-classical correlations (entanglement) between the two subsystems imply that the observables of one subsystem are determined by the measurement choice on the other, regardless of the distance between the subsystems. Nowadays, continuous-variable entanglement is regarded as an essential resource, allowing for quantum enhanced measurement resolution, the realization of quantum teleportation and quantum memories, or the demonstration of the Einstein-Podolsky-Rosen paradox. These applications rely on techniques to manipulate and detect coherences of quantum fields, the quadratures. Whereas in optics coherent homodyne detection of quadratures is a standard technique, for massive particles a corresponding method was missing. Here we report the realization of an atomic analogue to homodyne detection for the measurement of matter-wave quadratures. The application of this technique to a quantum state produced by spin-changing collisions in a Bose-Einstein condensate reveals continuous-variable entanglement, as well as the twin-atom character of the state. Our results provide a rare example of continuous-variable entanglement of massive particles. The direct detection of atomic quadratures has applications not only in experimental quantum atom optics, but also for the measurement of fields in many-body systems of massive particles.     

Generation of three-qubit entangled states using superconducting phase qubits

Entanglement is one of the key resources required for quantum computation, so the experimental creation and measurement of entangled states is of crucial importance for various physical implementations of quantum computers. In superconducting devices, two-qubit entangled states have been demonstrated and used to show violations of Bell's inequality and to implement simple quantum algorithms. Unlike the two-qubit case, where all maximally entangled two-qubit states are equivalent up to local changes of basis, three qubits can be entangled in two fundamentally different ways. These are typified by the states |GHZ>= (|000+?|111>)/ sqrt [2] and |W>= (|001>?+?|010>?+?|100>)/ sqrt [3]. Here we demonstrate the operation of three coupled superconducting phase qubits and use them to create and measure |GHZ> and |W>states. The states are fully characterized using quantum state tomography and are shown to satisfy entanglement witnesses, confirming that they are indeed examples of three-qubit entanglement and are not separable into mixtures of two-qubit entanglement.     

驱动单个原子制备纠缠相干态

提出一种利用经典场驱动单个原子与一个多模腔场相互作用制备腔场的多模纠缠相干态的方案.交替调整原子的跃迁频率,使原子与经典场及多模腔场交替作用,通过对原子的选态测量使多模腔场塌缩为多模纠缠相干态.     

快速造型（RP）／快速制造（RF）技术述评

简要介绍世界先进的快速造型（ＲＰ）及快速制造（ＲＦ）的工艺过程及特点。     

An efficient scheme for multi-party quantum state sharing via non-maximally entangled states

We present a new scheme for investigating the usefulness of non-maximally entangled states for multi-party quantum state shar-ing in a simple and elegant manner.In our scheme,the sender,Alice shares n various probabilistic channels composed of non-maximally entangled states with n agents in a network.Our protocol involves only Bell-basis measurements,single qubit measurements,and a two-qubit unitary transformation operated by free optional agents.Our scheme is a more convenient realiza-tion because no other multipartite joint measurements are needed.Furthermore,in our scheme various probabilistic channels lessen the requirement for quantum channels,which makes it more practical for physical implementation.     

量子区分与量子克隆简述

在经典信息理论中,编码状态可以精确复制与区分;而在量子信息中,由于态的叠加性存在,使得非正交态不可区分,量子态不可复制与删除.但是,量子态的区分和克隆在新型的量子信息科学中具有广泛的应用,例如量子密码的接收和窃听等.本文简要介绍量子态的区分和克隆的数学概念及相关研究结果.