Direct observation of electronic structure change by resistance random access memory effect in amorphous alumina

We measured X-ray absorption spectra of amorphous alumina with vacancy-type oxygen defects (AlOx) which exhibits the resistance random access memory (ReRAM) effect. We were able to detect changes in the electronic structure owing to the ReRAM effect. A major difference in the spectra near the O K-ab...

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Main Authors: Masato Kubota, Seisuke Nigo, Seiichi Kato, Kenta Amemiya
Format: Article
Language:English
Published: AIP Publishing LLC 2019-09-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.5086212
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spelling doaj-402397f94b454e048f0f8ca22080b7352020-11-25T00:59:04ZengAIP Publishing LLCAIP Advances2158-32262019-09-0199095050095050-410.1063/1.5086212072909ADVDirect observation of electronic structure change by resistance random access memory effect in amorphous aluminaMasato Kubota0Seisuke Nigo1Seiichi Kato2Kenta Amemiya3Japan Atomic Energy Agency (JAEA), 2-4 Shirakata Tokai-mura, Naka-gun, Ibaraki 319-1195, JapanInternational Center for Materials Nanoarchitectonics (MANA),National Institute for Materials Science (NIMS), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, JapanInternational Center for Materials Nanoarchitectonics (MANA),National Institute for Materials Science (NIMS), 1-1 Namiki, Tsukuba, Ibaraki 305-0044, JapanInstitute of Materials Structure Science, High Energy Accelerator Research Organization, Tsukuba, Ibaraki 305-0801, JapanWe measured X-ray absorption spectra of amorphous alumina with vacancy-type oxygen defects (AlOx) which exhibits the resistance random access memory (ReRAM) effect. We were able to detect changes in the electronic structure owing to the ReRAM effect. A major difference in the spectra near the O K-absorption edge was observed between a low resistance state (LRS) and a high resistance state (HRS). The subpeak profile within the band gap appeared in the LRS, while it was suppressed in the HRS. By contrast, the spectra near the Al K-absorption edge in the LRS and HRS appeared almost identical, indicating that no byproducts are generated. These findings imply that the distribution of charged electrons primarily changes near oxygen sites from the HRS to the LRS. The features of the subpeak profile are analogous to those of the mid-gap profile, as speculated by the first-principles calculation [Momida et al., Appl. Phys. Lett. 98, 042102 (2011)]. The LRS was mainly detected near the surface of the thin film.http://dx.doi.org/10.1063/1.5086212
collection DOAJ
language English
format Article
sources DOAJ
author Masato Kubota
Seisuke Nigo
Seiichi Kato
Kenta Amemiya
spellingShingle Masato Kubota
Seisuke Nigo
Seiichi Kato
Kenta Amemiya
Direct observation of electronic structure change by resistance random access memory effect in amorphous alumina
AIP Advances
author_facet Masato Kubota
Seisuke Nigo
Seiichi Kato
Kenta Amemiya
author_sort Masato Kubota
title Direct observation of electronic structure change by resistance random access memory effect in amorphous alumina
title_short Direct observation of electronic structure change by resistance random access memory effect in amorphous alumina
title_full Direct observation of electronic structure change by resistance random access memory effect in amorphous alumina
title_fullStr Direct observation of electronic structure change by resistance random access memory effect in amorphous alumina
title_full_unstemmed Direct observation of electronic structure change by resistance random access memory effect in amorphous alumina
title_sort direct observation of electronic structure change by resistance random access memory effect in amorphous alumina
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2019-09-01
description We measured X-ray absorption spectra of amorphous alumina with vacancy-type oxygen defects (AlOx) which exhibits the resistance random access memory (ReRAM) effect. We were able to detect changes in the electronic structure owing to the ReRAM effect. A major difference in the spectra near the O K-absorption edge was observed between a low resistance state (LRS) and a high resistance state (HRS). The subpeak profile within the band gap appeared in the LRS, while it was suppressed in the HRS. By contrast, the spectra near the Al K-absorption edge in the LRS and HRS appeared almost identical, indicating that no byproducts are generated. These findings imply that the distribution of charged electrons primarily changes near oxygen sites from the HRS to the LRS. The features of the subpeak profile are analogous to those of the mid-gap profile, as speculated by the first-principles calculation [Momida et al., Appl. Phys. Lett. 98, 042102 (2011)]. The LRS was mainly detected near the surface of the thin film.
url http://dx.doi.org/10.1063/1.5086212
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