Quantum State Transfer between Two Distant Atoms by Connecting Two Cavities via Optical Fibres

A scheme is proposed to unconditionally implement state transfer between two distant atoms by sending the atoms across two distant cavities connected via an optical fibre, respectively. The field state, which preserves the information about the first atom, is transmitted from one cavity to the other along the fibre. A Faraday rotator integrated in the fibre can be designed to completely stop the fields reflected from the second cavity, thus after the field interacts with the second atom for a defined time, the state transfer can be accomplished with unit efficiency.     

双原子非简并拉曼过程中原子与腔场的动力学

本文研究两原子与双模量子腔场的拉曼相互作用，分析原子反转度和腔场平均光子数的时间演化，考究腔场初态，初场强度以及原子间偶极相互作用的影响，并与单原子情况进行了比较，得到了一些新的有意义的结果。     

注入原子相干性对双模MAZER的影响

首先简单介绍超冷原子注入的微脉塞(MAZER)的基本理论和研究进展,然后具体介绍我们目前关于超冷V型三能级原子注入的双模微脉塞(双模MAZER)的研究工作.我们研究了原子相干性对这种双模MAZER系统中原子的发射几率和原子通过腔的透射几率的影响.结果表明,原子的发射几率随腔长变化的曲线中存在共振峰和非共振平台;当两个模的耦合强度之比一定时,不同注入原子相干性对应的发射几率共振峰呈现出相当大的区别.在原子透射几率随原子动量的变化曲线中也存在共振峰和非共振平台.腔长对原子的速度具有选择性,当腔长给定时,通过适当选择原子的相干参量,可调节原子通过腔的透射几率,从而可对原子的速度进行选择.     

拉普拉斯-龙格-楞次守恒量在天体运动中的应用

拉普拉斯-龙格-楞次(Laplace-Runge-Lenz)矢量虽然在大学物理教材上没有提及,但在物理竞赛中经常会涉及,本文简单介绍Laplace-Runge-Lenz守恒量,并通过一道竞赛物理题讲解其应用.     

基于腔输入-输出过程的原子Bell态分析器和GHZ态分析器

如何能够在不破坏纠缠态且能将其辨认区分出来是量子信息处理过程中一个很重要的问题,方案首先利用相干光与腔-原子系统的输入-输出过程构造受控相移门,然后利用受控相移门和零差探测技术构造宇称分析器,最后利用宇称分析器和Hadamard等操作构造非破坏性的原子Bell态分析器和原子GHZ态分析器。方案的优势在于:（1）利用到相干光源和零差探测技术,比以往方案中的单光子源和单光子探测较易实现;（2）构造的原子Bell态分析器和原子GHZ态分析器是非破坏性的。方案用到的所有方法和技术在目前的实验上都是可以实现的。     

利用微脉塞重构腔场的Wigner函数

提出了重构腔场Wigner函数的一种新方案.该方案可以用微脉塞来实现.发现在腔场的Wigner函数与原子的布居数之间存在一个简单的关系.在实验上测得原子的布居数后，进行一个简单的数值积分，就可得到腔场的Wigner函数.以单光子Fock态和Schr?dinger猫态为例进行了数值模拟，发现与用精确公式计算的结果很好地相符. 关键词： 量子态重构 Wigner函数 微脉塞     

基于腔辅助相互作用的远距离信息传递

提出了一种基于腔辅助相互作用的远距离信息传递的方案.在该方案中,通过让一束相干光和一个囚禁在腔里面的原子进行相互作用,可以使相干光产生一个可控的相位偏移.用这种腔辅助相互作用完成了原子态和光场态之间信息的相互转移.最后我们演示了远距离信息传递方案,该方案在当前实验条件下是可行的,并且在理想条件下,成功的概率几乎为1.     

Analytic solutions for degenerate Raman-coupled model

The Raman-coupled interaction between an atom and a single mode of a cavity field is studied. For the cases in which a light field is initially in a coherent state and in a thermal state separately, we have derived the analytic expressions for the time evolutions of atomic population difference W, modulus B of the Bloch vector, and entropy E. We find that the time evolutions of these quantities are periodic with a period of π. The maxima of W and B appear at the scaled interaction time points τ- = kπ（k = 0, 1, 2,...）. At these time points, E = 0, which shows that the atom and the field are not entangled. Between these time points, E ≠ 0, which means that the atom and the field are entangled. When the field is initially in a coherent state, near the maxima, the envelope of W is a Gaussian function with a variance of 1/（4n^-）（n^- is the mean number of photons）. Under the envelope, W oscillates at a frequency of n^-/π. When the field is initially in a thermal state, near the maxima, W is a Lorentz function with a width of 1/n^-.     

利用交叉克尔非线性效应实现纠缠转移

提出了一种基于交叉克尔非线性效应的纠缠态转移方案.利用该方案可以将离散变量光场态之间的纠缠关系转移到连续变量光场态(相干态)上.通过适当设置初始相干态的振幅，该方案可以使转移后的纠缠相干态处于最大纠缠态.     

A Scheme for Generating Entangled Squeezed States Based on Cavity QED

We propose a scheme for generating entangled squeezed vacuum states of electromagnetical fields. The scheme is based on cavity QED. In this scheme, an atom interacts, successively, with a classical field, two quantum cavity fields, and another classical field. By detecting the final states of the atom, the two quantum cavity fields will be projected to an entangled state.