Faraday laser at Rb 1529 nm transition for optical communication systems  被引量:1

Faraday laser at Rb 1529 nm transition for optical communication systems

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作  者:常鹏媛 史田田 张盛楠 商浩森 潘多 陈景标 

机构地区:[1]State Key Laboratory of Advanced Optical Communication System and Network, School of Electronics Engineering and Computer Science, Peking University, Beijing 100871, China

出  处:《Chinese Optics Letters》2017年第12期53-56,共4页中国光学快报(英文版)

基  金:supported by the National Natural Science Foundation of China under Grant No.91436210

摘  要:We experimentally demonstrate a Faraday laser at Rb 1529 nm transition by using a performance-improved Rb electrodeless-discharge-lamp-based excited-state Faraday anomalous dispersion optical filter as the frequency- selective element. Neither the electrical locking scheme nor the additional frequency-stabilized pump laser are used. The frequency of the external-cavity diode laser is stabilized to the Rb 1529 nm transition, and the Allan deviation of the Faraday laser is measured by converting the optical intensity into frequency. The Faraday laser can be used as a frequency standard in the telecom C band for further research on metrology, microwave photonics, and optical communication systems.We experimentally demonstrate a Faraday laser at Rb 1529 nm transition by using a performance-improved Rb electrodeless-discharge-lamp-based excited-state Faraday anomalous dispersion optical filter as the frequency- selective element. Neither the electrical locking scheme nor the additional frequency-stabilized pump laser are used. The frequency of the external-cavity diode laser is stabilized to the Rb 1529 nm transition, and the Allan deviation of the Faraday laser is measured by converting the optical intensity into frequency. The Faraday laser can be used as a frequency standard in the telecom C band for further research on metrology, microwave photonics, and optical communication systems.

关 键 词:Faraday laser at Rb 1529 nm transition for optical communication systems FADOF RB 

分 类 号:TN248[电子电信—物理电子学] TN929.1

 

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