Disentangling the Role of the SnO Layer on the Pyro‐Phototronic Effect in ZnO‐Based Self‐Powered Photodetectors

Self‐powered photodetectors (PDs) have been recognized as one of the developing trends of next‐generation optoelectronic devices. Herein, it is shown that by introducing a thin layer of SnO film between the Si substrate and the ZnO film, the self‐powered photodetector Al/Si/SnO/ZnO/ITO exhibits a st...

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Published in:Small (Weinheim an der Bergstrasse, Germany) Vol. 19; no. 32; pp. e2300607 - n/a
Main Authors: Vieira, Eliana M. F., Silva, José P. B., Gwozdz, Katarzyna, Kaim, Adrian, Gomes, Nuno M., Chahboun, Adil, Gomes, Maria J. M., Correia, José H.
Format: Journal Article
Language:English
Published: Germany Wiley Subscription Services, Inc 01-08-2023
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Summary:Self‐powered photodetectors (PDs) have been recognized as one of the developing trends of next‐generation optoelectronic devices. Herein, it is shown that by introducing a thin layer of SnO film between the Si substrate and the ZnO film, the self‐powered photodetector Al/Si/SnO/ZnO/ITO exhibits a stable and uniform violet sensing ability with high photoresponsivity and fast response. The SnO layer introduces a built‐in electrostatic field to highly enhance the photocurrent by over 1000%. By analyzing energy diagrams of the p‐n junction, the underlying physical mechanism of the self‐powered violet PDs is carefully illustrated. A high photo‐responsivity (R) of 93 mA W−1 accompanied by a detectivity (D*) of 3.1 × 1010 Jones are observed under self‐driven conditions, when the device is exposed to 405 nm excitation laser wavelength, with a laser power density of 36 mW cm−2 and at a chopper frequency of 400 Hz. The Si/SnO/ZnO/ITO device shows an enhancement of 3067% in responsivity when compared to the Al/Si/ZnO/ITO. The photodetector holds an ultra‐fast response of ≈ 2 µs, which is among the best self‐powered photodetectors reported in the literature based on ZnO. Self‐powered ZnO‐based photodetector with an optimum responsivity (R) and detectivity (D*)of 93 mA W−1 and 3.1 × 1010 Jones, respectively, for a laser power density of 36 mW cm−2 and a chopper frequency of 400 Hz. The SnO layer introduces a built‐in electrostatic field to highly enhance the photocurrent by over 1000%. Ultrafast rise and fall times of 2.2 and 2.0 µs, respectively, were obtained.
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ISSN:1613-6810
1613-6829
DOI:10.1002/smll.202300607