典型文献
Graphene photodetector employing double slot structure with enhanced responsivity and large bandwidth
文献摘要:
Silicon photonics integrated with graphene provides a promising solution to realize integrated photodetectors operating at the communication window thanks to graphene's ultrafast response and compatibility with CMOS fabrication process. However, current hybrid graphene/silicon photodetectors suffer from low responsivity due to the weak light-graphene in-teraction. Plasmonic structures have been explored to enhance the responsivity, but the intrinsic metallic Ohmic absorp-tion of the plasmonic mode limits its performance. In this work, by combining the silicon slot and the plasmonic slot wave-guide, we demonstrate a novel double slot structure supporting high-performance photodetection, taking advantages of both silicon photonics and plasmonics. With the optimized structural parameters, the double slot structure significantly promotes graphene absorption while maintaining low metallic absorption within the double slot waveguide. Based on the double slot structure, the demonstrated photodetector holds a high responsivity of 603.92 mA/W and a large bandwidth of 78 GHz. The high-performance photodetector provides a competitive solution for the silicon photodetector. Moreover, the double slot structure could be beneficial to a broader range of hybrid two-dimensional material/silicon devices to achieve stronger light-matter interaction with lower metallic absorption.
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作者姓名:
Siqi Yan;Yan Zuo;Sanshui Xiao;Leif Katsuo Oxenl?we;Yunhong Ding
作者机构:
DTU Electro,Department of Electrical and Photonics Engineering,Technical University of Denmark,Kgs.Lyngby DK-2800,Denmark;School of Optical and Electrical Information and Wuhan National Laboratory for Optoelectronics,Huazhong University of Science and Technology,Wuhan 430074,China.
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引用格式:
[1]Siqi Yan;Yan Zuo;Sanshui Xiao;Leif Katsuo Oxenl?we;Yunhong Ding-.Graphene photodetector employing double slot structure with enhanced responsivity and large bandwidth)[J].光电进展(英文版),2022(12):10-19
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0.511055
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