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用于光频传递的通信波段窄线宽激光器研制及应用
引用本文:焦东东,高静,刘杰,邓雪,许冠军,陈玖朋,董瑞芳,刘涛,张首刚.用于光频传递的通信波段窄线宽激光器研制及应用[J].物理学报,2015,64(19):190601-190601.
作者姓名:焦东东  高静  刘杰  邓雪  许冠军  陈玖朋  董瑞芳  刘涛  张首刚
作者单位:1. 中国科学院国家授时中心, 西安 710600; 2. 中国科学院大学, 北京 100049; 3. 中国科学院时间频率基准重点实验室, 西安 710600
基金项目:国家自然科学基金委重大科研仪器设备研制专项(批准号: 61127901), 国家自然科学基金(批准号: 11273024, 61025023), 国家自然科学基金青年科学基金(批准号: 11403031)、中组部“青年拔尖人才支持计划” 项目(批准号: 组厅字[2013]33 号)、中科院科技创新“交叉与合作团队” 项目(批准号: 中科院人教字(2012) 119 号)和中国科学院重点部署项目(批准号: KJZD-EW-W02)资助的课题.
摘    要:通信波段窄线宽激光器在基于光纤的光学频率传递中有着重要应用. 本文报道了1550 nm超窄线宽光纤激光器的研制及其在光学频率传递中的初步应用结果. 利用一台激光光源, 分别锁定到两个参考腔上(精细度分别为344000和296000), 锁定后经拍频比对测得单台激光线宽优于1.9 Hz, 秒级频率稳定度为1.7×10-14, 优于国内同类报道. 将研制的超窄线宽激光器用于光纤光学频率传递, 在50 km光纤盘上实现了 7.5×10-17/s的传递稳定度, 较采用商用光纤激光器提高了3.2倍.

关 键 词:时间频率  窄线宽激光  光学频率传递
收稿时间:2015-03-22

Development and application of communication band narrow linewidth lasers
Jiao Dong-Dong,Gao Jing,Liu Jie,Deng Xue,Xu Guan-Jun,Chen Jiu-Peng,Dong Rui-Fang,Liu Tao,Zhang Shou-Gang.Development and application of communication band narrow linewidth lasers[J].Acta Physica Sinica,2015,64(19):190601-190601.
Authors:Jiao Dong-Dong  Gao Jing  Liu Jie  Deng Xue  Xu Guan-Jun  Chen Jiu-Peng  Dong Rui-Fang  Liu Tao  Zhang Shou-Gang
Institution:1. National Time Service Centre, Chinese Academy of Sciences, Xi'an 710600, China; 2. University of Chinese Academy of Sciences, Beijing 100049, China; 3. Key Laboratory of Time and Frequency Standards, Chinese Academy of Sciences, Xi'an 710600, China
Abstract:Ultra-stable lasers at optical communication wavelengths have important applications in developing optical frequency transfer via optical fibers. We report the recent development of a 1550 nm stable laser system built at National Time Service Center and its preliminary application in optical frequency transfer via laboratory fibers. In the experiment, the conventional Pound-Drever-Hall(PDH) frequency stabilization technology is implemented to achieve the ultra-stable laser at the wavelength of 1550 nm. The output of a single laser source is split and locked onto the resonant frequency of two independent reference cavities, of 344000 and 296000 respectively. The frequency of the laser source is actively stabilized to the first reference cavity by piezo and external frequency shifters simultaneously and the total control bandwidth is measured to be 50 kHz. Then the laser frequency is shifted and stabilized to the second reference cavity by an acousto-optical modulator. A 5 m long single-mode fiber is used to bring the first laser beam to the second reference cavity which unfortunately induces unexpected phase noise by environmental distortions. The laser linewidth broadened is determined to be 0.27 Hz by the beat note measurement between the input and output beams of the fiber. To evaluate the frequency stability of the laser, the frequency control signal within the control bandwidth of the second stable laser system is analyzed by a spectrum analyzer and a frequency counter. The control signal shows a Lorentz linewidth of 2.7 Hz and a frequency stability of 2.5×10-14/s, corresponding to a single laser linewidth of 1.9 Hz with a frequency stability of 1.7×10-14/s if the two stable lasers have similar frequency stability. Applying this ultra-stable laser system as the laser source for the fiber-based optical frequency transfer, a short-term frequency transfer stability of 7.5×10-17/s is demonstrated through a 50 km-long fiber spool, while a frequency transfer stability of 2.4×10-16/s is achieved by a similar setup except that the laser source is a kHz-level linewidth laser. In the experiment an Agilent 53232 A frequency counter is applied to record the beat note signal in the auto mode. In the end, we discuss the possible improvements of the stable laser system, including the miniaturization of the optical setup, optimization of the control bandwidth and shortening of the response time of control loop.
Keywords:time and frequency  narrow linewidth laser  fiber optical frequency transfer
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