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Gain and bandwidth of InP nanowire array photodetectors with embedded photogated InAsP quantum discs
Halmstad University, School of Information Technology, Halmstad Embedded and Intelligent Systems Research (EIS). Lund University, Lund, Sweden.ORCID iD: 0000-0002-9939-2395
Halmstad University, School of Information Technology, Halmstad Embedded and Intelligent Systems Research (EIS). Lund University, Lund, Sweden.ORCID iD: 0000-0002-3160-8540
University of Kassel, Kassel, Germany.ORCID iD: 0000-0001-9705-9516
Lund University, Lund, Sweden.ORCID iD: 0000-0002-6269-2415
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2021 (English)In: Nanoscale, ISSN 2040-3364, E-ISSN 2040-3372, Vol. 13, no 12, p. 6227-6233Article in journal (Refereed) Published
Abstract [en]

Here we report on the experimental results and advanced self-consistent real device simulations revealing a fundamental insight into the non-linear optical response of n+-i-n+ InP nanowire array photoconductors to selective 980 nm excitation of 20 axially embedded InAsP quantum discs in each nanowire. The optical characteristics are interpreted in terms of a photogating mechanism that results from an electrostatic feedback from trapped charge on the electronic band structure of the nanowires, similar to the gate action in a field-effect transistor. From detailed analyses of the complex charge carrier dynamics in dark and under illumination was concluded that electrons are trapped in two acceptor states, located at 140 and 190 meV below the conduction band edge, at the interface between the nanowires and a radial insulating SiOx cap layer. The non-linear optical response was investigated at length by photocurrent measurements recorded over a wide power range. From these measurements were extracted responsivities of 250 A W-1 (gain 320)@20 nW and 0.20 A W-1 (gain 0.2)@20 mW with a detector bias of 3.5 V, in excellent agreement with the proposed two-trap model. Finally, a small signal optical AC analysis was made both experimentally and theoretically to investigate the influence of the interface traps on the detector bandwidth. While the traps limit the cut-off frequency to around 10 kHz, the maximum operating frequency of the detectors stretches into the MHz region. © The Royal Society of Chemistry

Place, publisher, year, edition, pages
Cambridge: Royal Society of Chemistry, 2021. Vol. 13, no 12, p. 6227-6233
National Category
Condensed Matter Physics
Identifiers
URN: urn:nbn:se:hh:diva-45953DOI: 10.1039/d1nr00846cISI: 000631583200001PubMedID: 33885608Scopus ID: 2-s2.0-85103624812OAI: oai:DiVA.org:hh-45953DiVA, id: diva2:1615018
Funder
EU, Horizon 2020, 641023Swedish Foundation for Strategic Research The Crafoord FoundationLund UniversityKnut and Alice Wallenberg Foundation, 2016.0089Swedish Research Council, 2018-04722Swedish Energy Agency, P38331-1
Note

The authors gratefully acknowledge financial support from NanoLund, the Swedish Research Council (project 2018-04722), the Swedish National Board for Industrial and Technological Development, the Knut and Alice Wallenberg Foundation (project 2016.0089), the Swedish Foundation for Strategic Research and the Swedish Energy Agency (project P38331-1), the Erik Johan Ljungberg Foundation, and the Crafoord Foundation. This project has also received funding from the European Union’s Horizon 2020 research and innovation program under Grant Agreement 641023 (NanoTandem). Finally, the authors acknowledge support from the National Center for High Resolution Electron Microscopy (nCHREM) at Lund University.

Available from: 2021-11-29 Created: 2021-11-29 Last updated: 2021-11-29Bibliographically approved

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Jeddi Abdarloo, HosseinKarimi, MohammadPettersson, Håkan

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