连续变量量子离物传态的实验研究

利用单个Ⅱ类相位匹配OPA产生的双模压缩态实现连续变量压缩纠缠态，完成了连续变量量 子离物传态. Ⅱ类相位匹配OPA参量反放大过程可以实现正交振幅反关联、正交位相关联的 压缩纠缠态，这不同于一般运转于阈值以下的OPO产生的正交振幅关联、正交位相反关联的 压缩纠缠态，可以采用直接平衡测量的方法完成Bell态测量. 利用双KTP补偿非线性过程的 离散效应，获得了最大压缩大于2dB的双模压缩纠缠态，实现保真度06，考虑到探测效率 实际保真度为057. 这种方案简化了测量方法与纠缠光源产生装置，有利于进行量子通信 的实验研究与应用. 同时，讨论了探测过程中的一些非理想因素. 关键词： 量子离物传态 压缩纠缠态 Bell态测量     

Stable Narrow Linewidth 689nm Diode Laser for the Second Stage Cooling and Trapping of Strontium Atoms

We report stable narrow linewidth laser systems based on self-developed Littman configuration external cavity diode lasers （ECDLs）. The frequency of the ECDL is stabilized to a high fineness ultralow-expansion glass reference cavity with the Pound-Drever-Hall technique. By heterodyne beating of two identical systems, we conclude that the linewidth 4.3× 10^-14 at an averaging measurement time. of each ECDL is reduced to lower than 150 Hz and its frequency stability reaches time of 1 s, the averaged long-term frequency drift is less than 0.2 Hz/s over 30 h     

自由空间量子通讯实验中纠缠源的研制

设计了适合自由空间量子通讯实验的纠缠源. 纠缠光子对的单模光纤搜集率约为每秒20000对,水平竖直方向的纠缠对比度大于95%,正负45°方向的纠缠对比度大于90%. 在本地得到了大于100个标准偏差的Bell 不等式破缺. 满足20 km量级的自由空间量子通讯试验要求. 关键词： 纠缠光子对 位相匹配 收集效率 贝尔不等式     

基于系数搜索的振动补偿方法

绝对重力仪普遍采用激光干涉式或原子干涉式的测量原理来测量重力加速度的绝对值,在地球物理等领域有着广泛的应用.振动补偿是一种有效减小地面振动对绝对重力仪测量精度的影响的方法,尤其适用于复杂振动环境.本文介绍了一种基于传递函数简化模型的、用于实时修正原子干涉式绝对重力仪干涉条纹的振动补偿方法,给出了该方法的工作原理及搜索模型系数的具体算法流程,然后利用仿真运算验证算法的有效性,最后利用已有的原子干涉式绝对重力仪对算法效果进行了实验评估.结果表明,使用该振动补偿算法对原子重力仪的干涉条纹进行修正,最大可将干涉条纹的余弦拟合残差的标准差衰减58%.该振动补偿算法具有较强的自适应性,有望提升原子干涉式绝对重力仪在不同测量环境尤其是复杂振动环境中的测量精度.     

在PPLN波导中利用上转换实现通讯波段单光子探测的研究

分析了在周期性极化铌酸锂(PPLN)波导中波长为1.32 μm和1.55 μm的光子和频过程.给出了达到最大信号转换效率所需要的泵浦光功率.分析了该过程中各种可能存在的噪声源,尤其是拉曼过程给出的噪声,给出了利用相干滤波片和标准具来减小噪声的方法.分析了该探测器在量子密码通讯中的应用.     

连续可调谐OPO及其在Cs2分子频率调制光谱中的应用

采用边带锁频技术,在II类相位匹配半整体光学参量振荡器(OPO)中实现双谐振OPO稳定单频运转,通过调谐抽运光频实现OPO输出连续可调谐, 最大连续调谐范围2.8GHz,将其应用于Cs2分子的频率调制光谱,观测到室温附近Cs2分子气室样品在1041.506nm附近的高分辨率光谱.     

二次谐波过程反射场的纠缠特性研究

本文从运动方程出发分析了三模共振条件下Ⅱ类相位匹配倍频过程中腔反射的泵浦场非经典特性.分别讨论了阈值以上、阈值以下两种情况下的稳态解.在此基础上分析了反射基频光正交分量的量子起伏特性,并结合实验参数计算了反射泵浦场两个垂直偏振模的量子纠缠特性,讨论了纠缠度与输出耦合、腔内损耗等参量的关系.     

A Hertz-Linewidth Ultrastable Diode Laser System for Clock Transition Detection of Strontium Atoms

The frequencies of two 698 nm external cavity diode lasers （ECDLs） are locked separately to two independently located ultrahigh finesse optical resonant cavities with the Pound Drever-Hall technique. The linewidth of each ECDL is measured to be -4.6 Hz by their beating and the fractional frequency stability below 5 × 10^-15 between 1 s to lOs averaging time. Another 698nm laser diode is injection locked to one of the cavity-stabilized ECDLs with a fixed frequency offset for power amplification while maintaining its linewidth and frequency characteristics. The frequency drift is H1 Hz/s measured by a femtosecond optical frequency comb based on erbium fiber. The output of the injection slave laser is delivered to the magneto-optical trap of a Sr optical clock through a iO- ta-long single mode polarization maintaining fiber with an active fiber noise cancelation technique to detect the clock transition of Sr atoms.     

Realization of Arbitrary Inverse Unitary Transformation of Single Mode Fibre by Using Three Wave Plates

We report a method to realize the arbitrary inverse unitary transformation imposed by a single-mode fibre on photon＇s polarization by the succession of two quarter-wave plates and a half-wave plate. The process of realization is analysed on a Poincar6 sphere due to the fact that unitary transformation does not change the angle formed by polarization state vector. The method is meaningful in quantum communication experiment such as quantum teleportation, in which an unknown arbitrary quantum state should be kept to be unchanged in the case of using a single-mode fibre for time delay.[第一段]     

Cooling and Trapping 88Sr Atoms with 461nm Laser

We report the experimental realization of a ^88Sr magneto-optical trap （MOT） operating at the wavelength of 461 nm. The MOT is loaded via a 32 cm long spin-flip type Zeeman slower which enhances the MOT population by a factor of 22. The total laser power available in our experiment is about 300mW. We have trapped 1.6 × 10^8 ^88 Sr atoms with a 679nm and 707nm repumping laser. The two repumping lasers enhance the trap population and trap lifetime by factors of 11 and 7, respectively. The ^88 Sr cloud has a temperature of about 2.3 mK, measured by recording the time evolution of the absorption signal.