Resistive Switching of GaAs Oxide Nanostructures

The paper presents the results of experimental studies of the influence of the local anodic oxidation control parameters on the geometric parameters of oxide nanoscale structures (ONS) and profiled nanoscale structures (PNS) on the surface of epitaxial structures of silicon doped gallium arsenide wi...

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Main Authors: Vadim Avilov, Nikita Polupanov, Roman Tominov, Maxim Solodovnik, Boris Konoplev, Vladimir Smirnov, Oleg Ageev
Format: Article
Language:English
Published: MDPI AG 2020-08-01
Series:Materials
Subjects:
Online Access:https://www.mdpi.com/1996-1944/13/16/3451
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author Vadim Avilov
Nikita Polupanov
Roman Tominov
Maxim Solodovnik
Boris Konoplev
Vladimir Smirnov
Oleg Ageev
author_facet Vadim Avilov
Nikita Polupanov
Roman Tominov
Maxim Solodovnik
Boris Konoplev
Vladimir Smirnov
Oleg Ageev
author_sort Vadim Avilov
collection DOAJ
description The paper presents the results of experimental studies of the influence of the local anodic oxidation control parameters on the geometric parameters of oxide nanoscale structures (ONS) and profiled nanoscale structures (PNS) on the surface of epitaxial structures of silicon doped gallium arsenide with an impurity concentration of 5 × 10<sup>17</sup> cm<sup>−3</sup>. X-ray photoelectron spectroscopy measurements showed that GaAs oxide consists of oxide phases Ga<sub>2</sub>O<sub>3</sub> and As<sub>2</sub>O<sub>3</sub>, and the thickness of the Ga<sub>2</sub>O<sub>3</sub> layer is 2–3 times greater than the thickness of As<sub>2</sub>O<sub>3</sub> area—i.e., the oxidized GaAs region consists mainly of Ga<sub>2</sub>O<sub>3</sub>. The experimental studies of the influence of ONS thickness on the resistive switching effect were obtained. An increase in the ONS thickness from 0.8 ± 0.3 to 7.6 ± 0.6 nm leads to an increase in the switching voltage <i>Uset</i> from 2.8 ± 0.3 to 6.8 ± 0.9 V. The results can be used in the development of technological processes for the manufacturing of nano-electronic elements, such as ReRAM, as well as a high-efficiency quantum dot laser.
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spelling doaj.art-39e5946dbfe24427849c658941d8d97d2023-11-20T09:09:50ZengMDPI AGMaterials1996-19442020-08-011316345110.3390/ma13163451Resistive Switching of GaAs Oxide NanostructuresVadim Avilov0Nikita Polupanov1Roman Tominov2Maxim Solodovnik3Boris Konoplev4Vladimir Smirnov5Oleg Ageev6Institute of Nanotechnologies, Electronics and Electronic Equipment Engineering, Southern Federal University, 347922 Taganrog, RussiaInstitute of Nanotechnologies, Electronics and Electronic Equipment Engineering, Southern Federal University, 347922 Taganrog, RussiaInstitute of Nanotechnologies, Electronics and Electronic Equipment Engineering, Southern Federal University, 347922 Taganrog, RussiaInstitute of Nanotechnologies, Electronics and Electronic Equipment Engineering, Southern Federal University, 347922 Taganrog, RussiaInstitute of Nanotechnologies, Electronics and Electronic Equipment Engineering, Southern Federal University, 347922 Taganrog, RussiaInstitute of Nanotechnologies, Electronics and Electronic Equipment Engineering, Southern Federal University, 347922 Taganrog, RussiaInstitute of Nanotechnologies, Electronics and Electronic Equipment Engineering, Southern Federal University, 347922 Taganrog, RussiaThe paper presents the results of experimental studies of the influence of the local anodic oxidation control parameters on the geometric parameters of oxide nanoscale structures (ONS) and profiled nanoscale structures (PNS) on the surface of epitaxial structures of silicon doped gallium arsenide with an impurity concentration of 5 × 10<sup>17</sup> cm<sup>−3</sup>. X-ray photoelectron spectroscopy measurements showed that GaAs oxide consists of oxide phases Ga<sub>2</sub>O<sub>3</sub> and As<sub>2</sub>O<sub>3</sub>, and the thickness of the Ga<sub>2</sub>O<sub>3</sub> layer is 2–3 times greater than the thickness of As<sub>2</sub>O<sub>3</sub> area—i.e., the oxidized GaAs region consists mainly of Ga<sub>2</sub>O<sub>3</sub>. The experimental studies of the influence of ONS thickness on the resistive switching effect were obtained. An increase in the ONS thickness from 0.8 ± 0.3 to 7.6 ± 0.6 nm leads to an increase in the switching voltage <i>Uset</i> from 2.8 ± 0.3 to 6.8 ± 0.9 V. The results can be used in the development of technological processes for the manufacturing of nano-electronic elements, such as ReRAM, as well as a high-efficiency quantum dot laser.https://www.mdpi.com/1996-1944/13/16/3451atomic force microscopylocal anodic oxidationgallium arsenideoxide nanoscale structureprofiled nanoscale structureeffect of resistive switching
spellingShingle Vadim Avilov
Nikita Polupanov
Roman Tominov
Maxim Solodovnik
Boris Konoplev
Vladimir Smirnov
Oleg Ageev
Resistive Switching of GaAs Oxide Nanostructures
Materials
atomic force microscopy
local anodic oxidation
gallium arsenide
oxide nanoscale structure
profiled nanoscale structure
effect of resistive switching
title Resistive Switching of GaAs Oxide Nanostructures
title_full Resistive Switching of GaAs Oxide Nanostructures
title_fullStr Resistive Switching of GaAs Oxide Nanostructures
title_full_unstemmed Resistive Switching of GaAs Oxide Nanostructures
title_short Resistive Switching of GaAs Oxide Nanostructures
title_sort resistive switching of gaas oxide nanostructures
topic atomic force microscopy
local anodic oxidation
gallium arsenide
oxide nanoscale structure
profiled nanoscale structure
effect of resistive switching
url https://www.mdpi.com/1996-1944/13/16/3451
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AT nikitapolupanov resistiveswitchingofgaasoxidenanostructures
AT romantominov resistiveswitchingofgaasoxidenanostructures
AT maximsolodovnik resistiveswitchingofgaasoxidenanostructures
AT boriskonoplev resistiveswitchingofgaasoxidenanostructures
AT vladimirsmirnov resistiveswitchingofgaasoxidenanostructures
AT olegageev resistiveswitchingofgaasoxidenanostructures