Electrostatically Induced Black Phosphorus Infrared Photodiodes

Author:

Yan Wei1ORCID,Wang Shifan1,Xing Kaijian2,Balendhran Sivacarendran1,Tebyetekerwa Mike3,Watanabe Kenji4,Taniguchi Takashi5,Fuhrer Michael S.26,Crozier Kenneth B.178,Bullock James1ORCID

Affiliation:

1. Department of Electrical and Electronic Engineering The University of Melbourne Parkville Victoria 3010 Australia

2. School of Physics and Astronomy Monash University Clayton Victoria 3800 Australia

3. School of Chemical Engineering The University of Queensland Brisbane Queensland 4072 Australia

4. Research Center for Electronic and Optical Materials National Institute for Materials Science 1‐1 Namiki Tsukuba 305‐0044 Japan

5. International Center for Materials Nanoarchitectonics National Institute for Materials Science 1‐1 Namiki Tsukuba 305‐0044 Japan

6. Australian Research Council Centre of Excellence in Future Low‐Energy Electronics Technologies (FLEET) Monash University Clayton Victoria 3800 Australia

7. School of Physics The University of Melbourne Parkville Victoria 3010 Australia

8. Australian Research Council (ARC) Centre of Excellence for Transformative Meta‐Optical Systems (TMOS) The University of Melbourne Parkville Victoria 3010 Australia

Abstract

AbstractHomojunctions are key elements in many mainstream electronic devices. However, conventional dopant‐based “pn” homojunctions are not easily achievable in new material families, such as the 2D materials. Several recent 2D material studies have shown that lateral pn homojunctions can instead be electrostatically induced using back gates localized to either the source or drain contacts. Here, a hBN‐encapsulated black phosphorus dual‐gate device containing a lateral pn homojunction, whose orientation can be switched via application of back gate voltages, is demonstrated. Importantly, this study extends the state‐of‐the‐art for this architecture by characterizing the photoresponse under infrared (λ = 2.2 µm) illumination. It is shown that when biased to form a homojunction, the device exhibits the photovoltaic effect, resulting in a specific detectivity of 8.5 × 108 cm Hz1/2 W−1 at 77 K under short‐circuit conditions, and an open circuit photovoltage up to 175 mV at 77 K. Further, it is shown that the device can be operated in photoconductive mode, allowing a high responsivity of 0.55 A W−1. This device is thus highly reconfigurable as it can be switched between photovoltaic and photoconductive modes of operation to prioritize low noise and fast response or high responsivity.

Funder

Australian Research Council

Publisher

Wiley

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