1.School of Electrical and Computer Engineering, Purdue University, West Lafayette, IN 47907, USA
2.Birck Nanotechnology Center, Purdue University, West Lafayette, IN 47907, USA
3.Department of Physics and Astronomy, Purdue University, West Lafayette, IN 47907, USA
4.Purdue Quantum Science and Engineering Institute (PQSEI), Purdue University, West Lafayette, IN 47907, USA
Alexandra Boltasseva (aeb@purdue.edu)
Vladimir M. Shalaev (shalaev@purdue.edu)
纸质出版日期:2020,
网络出版日期:2020-07-20,
收稿日期:2019-12-04,
修回日期:2020-05-27,
录用日期:2020-06-08
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Enhancing the graphene photocurrent using surface plasmons and a p-n junction[J]. LSA, 2020,9(4):1228-1237.
Wang, D. et al. Enhancing the graphene photocurrent using surface plasmons and a p-n junction. Light: Science & Applications, 9, 1228-1237 (2020).
Enhancing the graphene photocurrent using surface plasmons and a p-n junction[J]. LSA, 2020,9(4):1228-1237. DOI: 10.1038/s41377-020-00344-1.
Wang, D. et al. Enhancing the graphene photocurrent using surface plasmons and a p-n junction. Light: Science & Applications, 9, 1228-1237 (2020). DOI: 10.1038/s41377-020-00344-1.
The recently proposed concept of graphene photodetectors offers remarkable properties such as unprecedented compactness
ultrabroadband detection
and an ultrafast response speed. However
owing to the low optical absorption of pristine monolayer graphene
the intrinsically low responsivity of graphene photodetectors significantly hinders the development of practical devices. To address this issue
numerous efforts have thus far been made to enhance the light–graphene interaction using plasmonic structures. These approaches
however
can be significantly advanced by leveraging the other critical aspect of graphene photoresponsivity enhancement—electrical junction control. It has been reported that the dominant photocarrier generation mechanism in graphene is the photothermoelectric (PTE) effect. Thus
the two energy conversion mechanisms involved in the graphene photodetection process are light-to-heat and heat-to-electricity conversions. In this work
we propose a meticulously designed device architecture to simultaneously enhance the two conversion efficiencies. Specifically
a gap plasmon structure is used to absorb a major portion of the incident light to induce localized heating
and a pair of split gates is used to produce a p-n junction in graphene to augment the PTE current generation. The gap plasmon structure and the split gates are designed to share common key components so that the proposed device architecture concurrently realizes both optical and electrical enhancements. We experimentally demonstrate the dominance of the PTE effect in graphene photocurrent generation and observe a 25-fold increase in the generated photocurrent compared to the un-enhanced cases. While further photocurrent enhancement can be achieved by applying a DC bias
the proposed device concept shows vast potential for practical applications.
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