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Modeling of switching mechanism in GeSbTe chalcogenide superlattices

We study the switching process in chalcogenide superlattice (CSL) phase-change memory materials by describing the motion of an atomic layer between the low and high resistance states. Two models have been proposed by different groups based on high-resolution electron microscope images. Model 1 propo...

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Detalles Bibliográficos
Autores principales: Yu, Xiaoming, Robertson, John
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4518231/
https://www.ncbi.nlm.nih.gov/pubmed/26219904
http://dx.doi.org/10.1038/srep12612
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author Yu, Xiaoming
Robertson, John
author_facet Yu, Xiaoming
Robertson, John
author_sort Yu, Xiaoming
collection PubMed
description We study the switching process in chalcogenide superlattice (CSL) phase-change memory materials by describing the motion of an atomic layer between the low and high resistance states. Two models have been proposed by different groups based on high-resolution electron microscope images. Model 1 proposes a transition from Ferro to Inverted Petrov state. Model 2 proposes a switch between Petrov and Inverted Petrov states. For each case, we note that the main transition is actually a vertical displacement of a Ge layer through a Te layer, followed by a lateral motion of GeTe sublayer to the final, low energy structure. Through calculating energy barriers, the rate-determining step is the displacive transition.
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spelling pubmed-45182312015-08-06 Modeling of switching mechanism in GeSbTe chalcogenide superlattices Yu, Xiaoming Robertson, John Sci Rep Article We study the switching process in chalcogenide superlattice (CSL) phase-change memory materials by describing the motion of an atomic layer between the low and high resistance states. Two models have been proposed by different groups based on high-resolution electron microscope images. Model 1 proposes a transition from Ferro to Inverted Petrov state. Model 2 proposes a switch between Petrov and Inverted Petrov states. For each case, we note that the main transition is actually a vertical displacement of a Ge layer through a Te layer, followed by a lateral motion of GeTe sublayer to the final, low energy structure. Through calculating energy barriers, the rate-determining step is the displacive transition. Nature Publishing Group 2015-07-29 /pmc/articles/PMC4518231/ /pubmed/26219904 http://dx.doi.org/10.1038/srep12612 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
Yu, Xiaoming
Robertson, John
Modeling of switching mechanism in GeSbTe chalcogenide superlattices
title Modeling of switching mechanism in GeSbTe chalcogenide superlattices
title_full Modeling of switching mechanism in GeSbTe chalcogenide superlattices
title_fullStr Modeling of switching mechanism in GeSbTe chalcogenide superlattices
title_full_unstemmed Modeling of switching mechanism in GeSbTe chalcogenide superlattices
title_short Modeling of switching mechanism in GeSbTe chalcogenide superlattices
title_sort modeling of switching mechanism in gesbte chalcogenide superlattices
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4518231/
https://www.ncbi.nlm.nih.gov/pubmed/26219904
http://dx.doi.org/10.1038/srep12612
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