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利用多模波导的色模激发实现巨可调谐光色散

Giant tunable optical dispersion using chromo-modal excitation of a multimode waveguide.

作者信息

Diebold Eric D, Hon Nick K, Tan Zhongwei, Chou Jason, Sienicki Todd, Wang Chao, Jalali Bahram

机构信息

Electrical Engineering Department, University of California, Los Angeles, CA 90095, USA.

出版信息

Opt Express. 2011 Nov 21;19(24):23809-17. doi: 10.1364/OE.19.023809.

Abstract

The ability to control chromatic dispersion is paramount in applications where the optical pulsewidth is critical, such as chirped pulse amplification and fiber optic communications. Typically, devices used to generate large amounts (>100 ps/nm) of chromatic dispersion are based on diffraction gratings, chirped fiber Bragg gratings, or dispersion compensating fiber. Unfortunately, these dispersive elements suffer from one or more of the following restrictions: (i) limited operational bandwidth, (ii) limited total dispersion, (iii) low peak power handling, or (iv) large spatial footprint. Here, we introduce a new type of tunable dispersive device, which overcomes these limitations by leveraging the large modal dispersion of a multimode waveguide in combination with the angular dispersion of diffraction gratings to create chromatic dispersion. We characterize the device's dispersion, and demonstrate its ability to stretch a sub-picosecond optical pulse to nearly 2 nanoseconds in 20 meters of multimode optical fiber. Using this device, we also demonstrate single-shot, time-wavelength atomic absorption spectroscopy at a repetition rate of 90.8 MHz.

摘要

在诸如啁啾脉冲放大和光纤通信等光脉冲宽度至关重要的应用中,控制色散的能力至关重要。通常,用于产生大量(>100 ps/nm)色散的器件基于衍射光栅、啁啾光纤布拉格光栅或色散补偿光纤。不幸的是,这些色散元件存在以下一个或多个限制:(i)有限的工作带宽,(ii)有限的总色散,(iii)低峰值功率处理能力,或(iv)较大的空间占用。在此,我们引入了一种新型可调色散器件,它通过利用多模波导的大模态色散与衍射光栅的角色散相结合来产生色散,从而克服了这些限制。我们对该器件的色散进行了表征,并展示了其在20米多模光纤中将亚皮秒光脉冲展宽至近2纳秒的能力。使用该器件,我们还展示了重复频率为90.8 MHz的单次时间波长原子吸收光谱。

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