利用高质量单光子和光学腔实现延迟选择实验的方案

延迟选择实验是量子物理中一项重要的实验.本文利用单光子与腔的关系,提出了一种变通的可操作验证延迟选择实验方案.在光子进入腔中之后,通过控制光子与腔的失谐控制光子的入射(光子位于腔内)-反射(光子位于腔外)行为.该方案与传统的方案比较有一定的特点.     

基于矢量叠加实现差分编码的光子模数转换方案

提出并验证了一种基于矢量叠加原理对输入射频信号进行差分编码的光子模数转换方案.该方案采用两路不同波长脉冲源通过一个相位调制器对输入射频信号进行调制,调制输出接入延时线干涉仪从而产生两路具有固定相位差的差分调制信号.利用矢量叠加模块对两路差分调制信号的强度进行不同程度的衰减和组合,从而获得系统量化所需的各路传递函数之间的相移量.该方案能够对输入射频信号实现差分编码,有效提高了系统的比特精度.同时该方案结构简单,只需要一个相位调制器,一个延时线干涉仪和一个矢量叠加模块即可构建.另外,各路传递函数之间的相移量是通过衰减两路差分调制信号的强度来实现,避免了传统光子模数转换方案中调制器对温度、环境敏感而引入的相位漂移问题.本文对4比特模数转换系统进行了原理性验证,实验结果证实了基于矢量叠加原理的光子模数转换方案的可行性.     

基于PPKTP波导产生多通道光子对

提出了一种基于PPKTP波导利用自发参量产生多通道纠缠光子对的方案.计算在使用脉冲,连续激光,Ⅰ型、Ⅱ型相位匹配这些不同条件下,同时产生位于通信波段的多通道纠缠光子对的特性.结果显示该方案能够为量子密钥分配网络提供更为高效易行的方案.     

六光子超纠缠态制备方案

自发参量下转换对应于一种非线性光学过程, 实验上作为一种标准方法, 人们利用自发参量下转换源产生纠缠光子对. 本文考虑由自发参量下转换源产生三对纠缠光子的情况. 通过使用由几组偏振光 束分束器、分束器和半波片等线性光学器件组成的量子线路演化三对光子, 给出了一个高效制备 包含偏振纠缠和空间纠缠的六光子超纠缠态方案. 因为方案中包含了参量下转换源产生三对纠缠光子 的所有可能情况, 所以本方案有很高的效率. 基于弱非线性介质构建了一个量子非破坏性测量装置, 用于区分光子在两指定的空间模中的两种分布情况. 特别地, 方案中可以通过合理约束在量子非破坏性测量过程中引入的非线性强度来达到实际实验所限定的数量级, 因此, 该方案易于在实验上实现.     

基于数字微镜器件的光子计数对应鬼成像

提出了一种基于数字微镜器件的光子计数对应鬼成像方案。该方案采用数字微镜器件对光源进行调制,通过时间相关单光子计数技术获取光子计数值,并利用对应鬼成像算法计算目标物体的像。结合鬼成像理论和对应鬼成像理论阐明了光子计数对应鬼成像原理,并通过实验对该方案进行了验证。研究结果表明,该方案能够实现弱光成像。利用该方案可以获得与传统鬼成像效果相当的成像质量,但降低了图像重建过程中的计算量和算法复杂度。此外,该方案略去了阵列探测器对光强分布的测量,利用一个不具有空间分辨率的单光子探测器结合对应鬼成像算法,即可得目标物体的像,同时也能获得目标的距离信息。     

一种制备四光子相干态的新方案

本文提出了一种利用原子-腔场之间的Raman相会作用来制备四光子相干态的新方案.同样,还可以利用该方法制备八成分迭加态.     

单光子探测器量子效率绝对自身标定方案

参考已有的方案,提出了一种更简单的方案来实现单光子探测器量子效率的绝对自身标定。我们利用同轴线缆和数据采集卡代替已有方案中的符合测量电路和计数器,通过精确设定同轴线缆的长度,利用电脉冲在同轴线缆的短路终端反射回波的特性,对一个测量周期中单个脉冲和连续两个脉冲进行区分,用数据采集卡记录区分结果,分别得到探测器探测到两个孪生光子的计数和仅探测到其中任意一个光子的计数,从而算出单光子探测器的量子效率。此方案不需要其他任何的参考标准或者另一个探测器.     

三粒子纠缠相干态的隐形传态

提出了一个利用一个两粒子最大纠缠相干态和一个三粒子纠缠相干态作为量子信道进行三粒子纠缠相干态隐形传态的方案.该方案只需线性光学操作和双模光子数测量.计算结果表明,应用本方案的设置,隐形传态成功的概率与所用的相干态的平均光子数有关,反映了纠缠相干态的非正交特性.     

基于部分纠缠光子源的高效量子密钥分配方案

设计了一种高效的部分纠缠光子对产生装置,这套装置中使用了简单的线性光学元件以及双光子吸收介质(TPAM),在文中讨论了TPAM的一种实现方案.我们把此种装置应用于量子密钥分配方案,分析了其效率和安全性,相比于用自发参量下转换(SPDC)产生纠缠光子对的密钥分配方案,该方案有更高的效率和安全性.     

基于两光子宇称门接近确定性的制备偏振Cluster态(英文)EI北大核心CSCD

基于弱的交叉克尔效应和线性光学元件,利用光子偏振宇称门呈现了一个关于制备Cluster态的方案.本方案引入了交叉克尔非线性介质,采用了对相干探测模的非破坏测量,有效实现了光子与光子间的相互作用,进而获得所期望的光子纠缠态,同时可以提高制备的成功概率和制备态的保真度.通过本方案可以制备接近完美保真度的四光子偏振Cluster态,并具有接近1的成功概率.在本方案的基础上通过利用线性光学元件还可以获得3N+1个光子的偏振Cluster态.     

Secure quantum dialogue based on single-photon

In this paper a quantum dialogue scheme is proposed by using N batches of single photons. The same secret message is encoded on each batch of single photons by the sender with two different unitary operations, and then the N batches of single photons are sent to the receiver. After eavesdropping check, the message is encoded on the one remaining batch by the receiver. It is shown that the intercept-and-resend attack and coupling auxiliary modes attack can be resisted more efficiently, because the photons are sent only once in our quantum dialogue scheme.     

基于自发参量下转换源二阶激发过程产生四光子超纠缠态

目前,多光子纠缠态的制备大多通过线性光学器件演化自发参量下转换一阶激发过程产生的纠缠光子对得到.本文考虑由自发参量下转换源二阶激发产生四个不可区分的纠缠光子制备四光子超纠缠态的情况.通过几组分束器、半波片和偏振分束器等线性光学器件设计量子线路演化四光子系统,结合四模符合探测,可得到同时具有偏振纠缠和空间纠缠的四光子超纠缠态.     

Production of Three-Dimensional Maximal Entanglement for Two Cavity Modes

A scheme is proposed for generating maximally entangled states for two cavity modes, with each containing no more than two photons. In the scheme a single atom is sent through two resonant single-mode cavities. Based on the presently available techniques, our scheme might be experimentally realizable.     

制备n原子GHZ类态

我们提出一个方案通过极化光子的干涉来制备囚禁在相距很远的腔中的n原子GHZ类态。在该方案中,原子腔耦合强度小于腔衰减率。因此对腔的品质因子的要求大大降低了,而且,该方案的保真度不受探测器效率和原子自发衰变的影响。 中文关键词：纠缠制备;GHZ类态;腔QED     

Teleportation of Multi-ionic GHZ States and Arbitrary Bipartite Ionic State via Linear Optics

We present a scheme for teleportation of multi-ionic GHZ states and arbitrary bipartite ionic state only by single-qubit measurements via linear optical elements. In our scheme, we avoid the difficulty of joint measurement and synchronizing the arrival time of the two scattered photons, which are faced by previous schemes. So our scheme can be realized easily within current experimental technology.     

Quantum State Transfer via Adiabatic Passage

我们采用周期极化KTP晶体为非线性介质，通过光学参量振荡器运转于阈值以下的简并参量振荡过程，产生了单模正交压缩真空态光场，在泵浦功率为123mW，Local光功率为842uW，晶体温度为32．1摄氏度时我们使用平衡零拍探测法测得输出场噪声功率低于散粒噪声基准3．41dB。     

Quantum state transfer via adiabatic passage

Based on adiabatic passage, we propose a scheme for implementing the quantum transfer of an unknown atomic state. In our scheme, we utilize photons for ideal quantum transmission between two cavities with the successful probability being about 1. Meanwhile, the scheme is robust against the effects of atomic spontaneous emission. It may be useful for transferring quantum information among spatially distant atoms.     

A probabilistic quantum communication protocol using mixed entangled channel

Qubits are realized as polarization state of photons or as superpositions of the spin states of electrons. In this paper we propose a scheme to probabilistically teleport an unknown arbitrary two-qubit state using a non-maximally entangled GHZ-like state and a non-maximally Bell state simultaneously as quantum channels. We also discuss the success probability of our scheme. We perform POVM in the protocol which is operationally advantageous. In our scheme we show that the non-maximal quantum resources perform better than maximal resources.     

High-Capacity Three-Party Quantum Secret Sharing With Hyperentanglement

We presents a novel scheme for high-capacity three-party quantum secret sharing (QSS) with the hyperentanglement in both the polarization and the spatial-mode degrees of freedom of photon pairs. The boss Alice need only prepare a sequence of photon pairs and some decoy photons. Her two agents measure their photons received from the boss Alice with two bases by choosing two unsymmetrical probabilities. The present QSS scheme has a high capacity as each pair can carry 2 bits of information, several times as other QSS schemes. Moreover, our setups with linear optical elements show that our QSS scheme does not increase the difficulty of its implementation in experiment and it is feasible with current techniques.     

An Efficient Scheme for Entanglement Concentration of Arbitrary Four-Photon States

The maximally entanglement will become less-entangled state because of the effects of decoherence. However, maximally entangled states are usually important for most of the quantum information processing protocols. So we propose a practical entanglement concentration protocol of an arbitrary four-photon less-entangled state assisted with single photons, which greatly reduces the difficulty of the experimental realization. In our scheme, we only employ three steps, a four-photon cluster state can be acquired with a certain probability by three affiliated photons. The protocol adopts the linear optical elements and weak cross-Kerr media, which make the scheme more simple and feasible in the experiment.