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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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 |
work_keys_str_mv |
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