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Thickness effect of ultra-thin Ta(2)O(5) resistance switching layer in 28 nm-diameter memory cell

Resistance switching (RS) devices with ultra-thin Ta(2)O(5) switching layer (0.5–2.0 nm) with a cell diameter of 28 nm were fabricated. The performance of the devices was tested by voltage-driven current—voltage (I-V) sweep and closed-loop pulse switching (CLPS) tests. A Ta layer was placed beneath...

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Autores principales: Park, Tae Hyung, Song, Seul Ji, Kim, Hae Jin, Kim, Soo Gil, Chung, Suock, Kim, Beom Yong, Lee, Kee Jeung, Kim, Kyung Min, Choi, Byung Joon, Hwang, Cheol Seong
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4630583/
https://www.ncbi.nlm.nih.gov/pubmed/26527044
http://dx.doi.org/10.1038/srep15965
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author Park, Tae Hyung
Song, Seul Ji
Kim, Hae Jin
Kim, Soo Gil
Chung, Suock
Kim, Beom Yong
Lee, Kee Jeung
Kim, Kyung Min
Choi, Byung Joon
Hwang, Cheol Seong
author_facet Park, Tae Hyung
Song, Seul Ji
Kim, Hae Jin
Kim, Soo Gil
Chung, Suock
Kim, Beom Yong
Lee, Kee Jeung
Kim, Kyung Min
Choi, Byung Joon
Hwang, Cheol Seong
author_sort Park, Tae Hyung
collection PubMed
description Resistance switching (RS) devices with ultra-thin Ta(2)O(5) switching layer (0.5–2.0 nm) with a cell diameter of 28 nm were fabricated. The performance of the devices was tested by voltage-driven current—voltage (I-V) sweep and closed-loop pulse switching (CLPS) tests. A Ta layer was placed beneath the Ta(2)O(5) switching layer to act as an oxygen vacancy reservoir. The device with the smallest Ta(2)O(5) thickness (0.5 nm) showed normal switching properties with gradual change in resistance in I-V sweep or CLPS and high reliability. By contrast, other devices with higher Ta(2)O(5) thickness (1.0–2.0 nm) showed abrupt switching with several abnormal behaviours, degraded resistance distribution, especially in high resistance state, and much lower reliability performance. A single conical or hour-glass shaped double conical conducting filament shape was conceived to explain these behavioural differences that depended on the Ta(2)O(5) switching layer thickness. Loss of oxygen via lateral diffusion to the encapsulating Si(3)N(4)/SiO(2) layer was suggested as the main degradation mechanism for reliability, and a method to improve reliability was also proposed.
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spelling pubmed-46305832015-11-05 Thickness effect of ultra-thin Ta(2)O(5) resistance switching layer in 28 nm-diameter memory cell Park, Tae Hyung Song, Seul Ji Kim, Hae Jin Kim, Soo Gil Chung, Suock Kim, Beom Yong Lee, Kee Jeung Kim, Kyung Min Choi, Byung Joon Hwang, Cheol Seong Sci Rep Article Resistance switching (RS) devices with ultra-thin Ta(2)O(5) switching layer (0.5–2.0 nm) with a cell diameter of 28 nm were fabricated. The performance of the devices was tested by voltage-driven current—voltage (I-V) sweep and closed-loop pulse switching (CLPS) tests. A Ta layer was placed beneath the Ta(2)O(5) switching layer to act as an oxygen vacancy reservoir. The device with the smallest Ta(2)O(5) thickness (0.5 nm) showed normal switching properties with gradual change in resistance in I-V sweep or CLPS and high reliability. By contrast, other devices with higher Ta(2)O(5) thickness (1.0–2.0 nm) showed abrupt switching with several abnormal behaviours, degraded resistance distribution, especially in high resistance state, and much lower reliability performance. A single conical or hour-glass shaped double conical conducting filament shape was conceived to explain these behavioural differences that depended on the Ta(2)O(5) switching layer thickness. Loss of oxygen via lateral diffusion to the encapsulating Si(3)N(4)/SiO(2) layer was suggested as the main degradation mechanism for reliability, and a method to improve reliability was also proposed. Nature Publishing Group 2015-11-03 /pmc/articles/PMC4630583/ /pubmed/26527044 http://dx.doi.org/10.1038/srep15965 Text en Copyright © 2015, Macmillan Publishers Limited http://creativecommons.org/licenses/by/4.0/ This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/
spellingShingle Article
Park, Tae Hyung
Song, Seul Ji
Kim, Hae Jin
Kim, Soo Gil
Chung, Suock
Kim, Beom Yong
Lee, Kee Jeung
Kim, Kyung Min
Choi, Byung Joon
Hwang, Cheol Seong
Thickness effect of ultra-thin Ta(2)O(5) resistance switching layer in 28 nm-diameter memory cell
title Thickness effect of ultra-thin Ta(2)O(5) resistance switching layer in 28 nm-diameter memory cell
title_full Thickness effect of ultra-thin Ta(2)O(5) resistance switching layer in 28 nm-diameter memory cell
title_fullStr Thickness effect of ultra-thin Ta(2)O(5) resistance switching layer in 28 nm-diameter memory cell
title_full_unstemmed Thickness effect of ultra-thin Ta(2)O(5) resistance switching layer in 28 nm-diameter memory cell
title_short Thickness effect of ultra-thin Ta(2)O(5) resistance switching layer in 28 nm-diameter memory cell
title_sort thickness effect of ultra-thin ta(2)o(5) resistance switching layer in 28 nm-diameter memory cell
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4630583/
https://www.ncbi.nlm.nih.gov/pubmed/26527044
http://dx.doi.org/10.1038/srep15965
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