Abstract

Abstract Recent discoveries in the field of graphene-based heterostructures have led to the demonstration of high-performance photodetectors. However, the studies to date have been largely limited to the heterojunction with a Schottky barrier, restricted by an inevitable compromise between photoresponsivity and photodetectivity. Here, a new class of graphene-based tunneling photodetectors is introduced by inserting the Al2O3 tunneling layer between silicon and graphene. The photocarriers can tunnel through the designed insulator layer which simultaneously blocks the dark current, thus maintaining high photodetectivity with desirable photoresponsivity. We further modulate the thickness of the Al2O3 layer to explore the tunneling mechanism for the photocarriers, in which a photoresponsivity of 0.75 A/W, a high current ratio of 4.8 × 103 and a photodetectivity of 3.1 × 1012 Jones are obtained at a 13.3-nm-thick Al2O3 layer. In addition, the fabrication process is compatible with conventional semiconductor processing, providing further flexibility to large-scale integrated photodetectors with high performance.

Highlights

  • Due to its unique structure, high carrier mobility and novel optical properties, graphene has been demonstrated as a promising material in optoelectronics that triggers extensive application prospect in photodetection [1,2,3,4]

  • Recent discoveries in the field of graphene-based heterostructures have led to the demonstration of high-performance photodetectors

  • A planar phototransistor based on graphene/Ti2O3 can acquire a high responsivity of 300 A/W as the trapped photogenerated carriers provide an additional electric field, while the photodetectivity falls to ~108 Jones [18]

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Summary

Introduction

Due to its unique structure, high carrier mobility and novel optical properties, graphene has been demonstrated as a promising material in optoelectronics that triggers extensive application prospect in photodetection [1,2,3,4]. We further modulate the thickness of the Al2O3 layer to explore the tunneling mechanism for the photocarriers, in which a photoresponsivity of 0.75 A/W, a high current ratio of 4.8 × 103 and a photodetectivity of 3.1 × 1012 Jones are obtained at a 13.3-nmthick Al2O3 layer.

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