Author Affiliations
Abstract
Key Laboratory on Luminescence and Optical Information Technology, Ministry of Education, Beijing Jiaotong University, Beijing 100044, China
We report a new method to deeply analyze the scrambling characteristic of polarization scramblers based on density of polarization states (DPS) statistics that makes it possible to describe the DPS distribution in detail on the whole Poincaré sphere, thus easy to locate accurately the nonuniform areas of defective polarization scramblers, which cannot be realized by existing methods. We have built a polarization scrambling system to demonstrate the advantages of our method compared with others by experiments and suggested effective evaluation indexes whose validity is well confirmed by applying to a commercial scrambler. Our conclusions are valuable for accurately analyzing and diagnosing the performance of any polarization scrambler, and quality evaluation of polarization controllers or other polarization devices.
optical communication polarization scrambling density of polarization states 
Chinese Optics Letters
2020, 18(6): 060604
Author Affiliations
Abstract
Key Laboratory of Luminescence and Optical Information Technology, Ministry of Education, Beijing Jiaotong University, Beijing 100044, China
We propose and demonstrate a novel scheme of semi-open-loop polarization control (SOL-PC), which controls the state of polarization (SOP) with high accuracy and uniform high speed. For any desired SOP, we first adjust the initial SOP using open-loop control (OLC) based on the matrix model of a three-unit piezoelectric polarization controller, and quickly move it close to the objective one. Then closed-loop control (CLC) is performed to reduce the error and reach precisely the desired SOP. The response time is three orders faster than that of the present closed-loop polarization control, while the average deviation is on par with it. Finally, the SOL-PC system is successfully applied to realize the suppression of the polarization mode dispersion (PMD) effect and reduce the first-order PMD to near zero. Due to its perfect performance, the SOL-PC energizes the present polarization control to pursue an ideal product that can meet the future requirements in ultrafast optical transmission and quantum communication.
polarization control polarization mode dispersion fiber optics components coherent communications 
Chinese Optics Letters
2020, 18(5): 050601
Author Affiliations
Abstract
1 Key Lab of Education Ministry on Luminescence and Optical Information Technology, Beijing Jiaotong University, Beijing 100044, China
2 The Institute of Optics, University of Rochester, 275 Hutchison Road, Rochester, New York 14627, USA
We demonstrate an ultralow-noise single-photon detection system based on a sensitive photomultiplier tube (PMT) with precise temperature control, which can capture fast single photons with intervals around 10 ns. By improvement of the electromagnetic shielding and introduction of the self-differencing method, the dark counts (DCs) are cut down to 1%. We further develop an ultra-stable PMT cooling subsystem and observe that the DC goes down by a factor of 3.9 each time the temperature drops 10°C. At 20°C it is reduced 400 times with respect to the room temperature (25°C), that is, it becomes only 2 counts per second, which is on par with the superconducting nanowire detectors. Meanwhile, despite a 50% loss, the detection efficiency is still 13%. Our detector is available for ultra-precise single-photon detection in environments with strong electromagnetic disturbances.
030.5260 Photon counting 
Chinese Optics Letters
2017, 15(10): 100301
作者单位
摘要
北京交通大学 发光与光信息技术教育部重点实验室, 北京100044
随着光学操控技术的迅速发展, 测量与重建径向偏振光束(RPB)成为迫切任务之一。利用一套石英旋光片组合, 首先产生了RPB。借助计算机控制的CCD, 对RPB的斯托克斯矢量场分布进行了测量, 并获得其偏振态分布。结果表明: 所产生的RPB归一化功率偏差为0.054 8, 偏振偏差为0.004 4。利用干涉仪, 获得了RPB的相位分布, 相邻断面间平均相位差为1.471。最后, 通过偏振和相位信息的数据处理, 成功重建了RPB的矢量场分布, 并发现其拓扑荷在3左右。这些结论为实现精密量子调控与测量铺平了道路。
径向偏振光束 斯托克斯矢量 干涉仪 光场重建 radially polarized beams Stokes vector interferometer optical field reconstructing 
红外与激光工程
2017, 46(4): 0427002
Author Affiliations
Abstract
1 Key Laboratory of Education Ministry on Luminescence and Optical Information Technology, Beijing Jiaotong University, Beijing 100044, China
2 Institute of Optical Information, School of Science, Beijing Jiaotong University, Beijing 100044, China
Polarization-based optical communications are attracting more attention recently, where the crucial points are polarization features and their measurements. Based on the Müller matrix method, we obtain measurable expressions for the polarization-dependent gain (PDG) and the loss of polarization orthogonality (LPO), while give the boundary of the LPO for any PDG devices. We experimentally demonstrate that non-linear LPO can be created in a semiconductor optical amplifier and find that the LPO will slightly skim over the boundary near the threshold of the injected current. Furthermore, an empirical formula is achieved to gauge the LPO-induced power penalty, which is proven to be valid in differential polarization shift-keying transmission by executing a bit error rate measurement. Our conclusions are applicable to non-orthogonal polarization cases and valuable to polarization-related communications, even orbital angular momentum multiplexing.
060.2330 Fiber optics communications 260.5430 Polarization 060.2340 Fiber optics components 
Chinese Optics Letters
2016, 14(9): 090601
Author Affiliations
Abstract
Key Laboratory of Luminescence and Optical Information, Ministry of Education, Institute of Optical Information, Beijing Jiaotong University, Beijing 100044, China
Quasi-single-photon sources are attracting a lot of interest in many fields at present; however, the knowledge is very poor about their performance. In this Letter, by using the standard Hanbury-Brown-Twiss measurement method, we investigate in detail the characteristics of the photons from an attenuated continuous single-mode red laser. For the first time to our knowledge we obtain the coincidence counting spectrum of a commercial single-photon source, which demonstrates that an appropriately attenuated continuous laser can be utilized as a quasi-single-photon source for general applications.
Chinese Optics Letters
2015, 13(Suppl): S20301
作者单位
摘要
1 北京交通大学发光与光信息技术教育部重点实验室, 北京 100044
2 北京交通大学理学院光信息科学与技术研究所, 北京 100044
3 重庆光电技术研究所, 重庆 400060
偏振编码器的稳定性是影响偏振编码通信的关键因素之一。采用时变矢量对基于铌酸锂(LN)相位调制的偏振编码器的稳定性进行了深入研究。实验表明,LN的偏振相关损耗主态(PPL)与偏振相关相移主态基本一致,说明LN的偏振相关损耗不会影响偏振态的稳定性。实验中观察到偏振态旋转具有“惯性”:使电压从0增加到某个定值,在停止增加后,偏振态会继续变化一段时间,大约在30 min后才达到稳定;相反,使电压从某个定值减少为0,在停止减少后,偏振态仍会继续变化一段时间。该现象对于低速调制将带来不利影响;对于高速调制,平均功率的变化也将引起偏振抖动。
光纤光学 光纤器件 偏振编码通信 偏振编码器 稳定性 
光学学报
2014, 34(9): 0906004
作者单位
摘要
北京交通大学理学院光信息科学与技术研究所, 发光与光信息技术教育部重点实验室, 北京 100044
各态遍历偏振态发生器(PSG)是偏振测量不可或缺的基本设备,偏振态和偏振器件的描述对于编写偏振态发生器的控制算法是至关重要的。采用四元数来描述和分析各态遍历偏振态发生器中偏振态与偏振控制器,导出了三级偏振控制器的四元数公式,得到了描述其旋转轴与旋转角度的公式。实验测量了单级偏振控制器的四元数,得到了普通单模光纤受挤压时对应的应力四元数公式以及改变电压时的四元数公式,利用该公式编制的算法,实现了各态遍历的偏振态发生器。
光纤光学 偏振态发生器 各态遍历 四元数 偏振旋转 
光学学报
2014, 34(3): 0306002
作者单位
摘要
北京交通大学光信息科学与技术研究所,教育部发光与光信息技术重点实验室, 北京 100044
半导体光放大器(SOA)因其具有良好的光-光互作用特性,包括交叉增益调制、交叉相位调制、交叉偏振调制以及四波混频等,在全光信号处理技术中已经获得了广泛的应用。利用SOA与光纤反馈可构成环形腔激光器S-FRL。在S-FRL中将SOA的光-光互作用特性与反馈条件相结合,可以改变S-FRL的起振、抑制、选频等多种状态,从而构成不同功能的全光信号处理器件。在分析S-FRL激光振荡原理的基础上,提出了双环耦合的S-FRL,并以此为基础构成一种双环耦合的双稳态触发器,进而构成一种同步脉冲展宽器;还提出了一种级联的S-FRL,由此构成一种基于负逻辑的全光判决器。
半导体光放大器 环形腔激光器 全光信号处理 双稳态触发器 同步脉冲展宽器 全光判决器 semiconductor optical amplifier fiber ring laser all-optical signal processing bi-stable optical flip-flop synchronous pulse broadening device optical decision 
光学与光电技术
2012, 10(5): 6
作者单位
摘要
1 北京交通大学 发光与光信息技术教育部重点实验室
2 光信息研究所, 北京 100044
环境温度变化和振动会引起光纤马赫曾德干涉仪两臂相差随机性变化, 致使干涉仪输出不稳定.本文研究了自然条件下外界温度和振动对基于3×3耦合器干涉仪的影响, 分析结果表明, 温度和振动所引起的干扰主要集中于100 Hz以下的低频成分中.为了消除这些干扰, 设计了单臂补偿的反馈回路以稳定输出信号, 并提出了一种利用象限判决方法来区分反馈正负性的动态补偿方法.实验中利用3×3耦合器3个输出端中其中2个进行光电变换、差分放大等反馈电路后驱动管状压电陶瓷, 使缠绕在其上的光纤伸缩, 动态补偿干涉仪相差的漂移, 稳定干涉仪输出即3×3耦合器第三输出端口的信号.针对自然环境下温度和振动引起的干扰, 本文研制了一种稳定的动态补偿装置, 能有效抑制160 Hz以下的低频干扰, 实时补偿干涉仪两臂的相差漂移, 干涉仪输出稳定的干涉信号, 波动幅度小于5.64%.
光纤马赫曾德干涉仪 3×3耦合器 相位补偿 反馈 稳定性 Optical fiber MachZehnder interferometer 3×3 coupler Phase compensation Feedback Stabilization 
光子学报
2012, 41(9): 1041

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