Outlooks for development of silicon nanoparticle memory cells

Phase change memory is based on changes in the optical, electrical or other properties of materials during phase transitions, e.g. an amorphous to crystalline transition. Currently existing and potential applications of this memory are primarily based on multicomponent alloys of meta...

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Main Authors: Igor V. Talyzin, Vladimir M. Samsonov
Format: Article
Language:English
Published: Pensoft Publishers 2019-12-01
Series:Modern Electronic Materials
Online Access:https://moem.pensoft.net/article/51788/download/pdf/
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spelling doaj-df8a77f552644a7badfe93bf366df9fb2021-04-02T07:46:30ZengPensoft PublishersModern Electronic Materials2452-17792019-12-015415916410.3897/j.moem.5.4.5178851788Outlooks for development of silicon nanoparticle memory cellsIgor V. Talyzin0Vladimir M. Samsonov1Tver State UniverTver State Univer Phase change memory is based on changes in the optical, electrical or other properties of materials during phase transitions, e.g. an amorphous to crystalline transition. Currently existing and potential applications of this memory are primarily based on multicomponent alloys of metals and semiconductors. However single-component nanoparticles including Si ones are also of interest as promising nanosized memory cells. The potential for developing this type of memory cells is confirmed by the fact that the optical absorption index of bulk amorphous silicon is of the same order of magnitude as that of crystalline silicon. Certainly this phenomenon can hardly be implemented with a single nanoparticle the size of which is within light wavelength. Using molecular dynamics and the Stillinger-Weber potential we have studied the regularities of melting and the conditions of crystallization of silicon nanoparticles containing within 105 atoms. We have shown that cooling of nanosized silicon drops at a 0.2 TK/s rate or higher rates causes their amorphous transition whereas single-component nanosized metallic drops crystallize in molecular dynamics experiments even at a 1 TK/s rate. Further heating of amorphous silicon nanoparticles containing above 5 ∙ 104 atoms causes their crystallization in a specific temperature range from 1300 to 1400 K. We have concluded that there is a possibility of developing phase change memory cells on the basis of the above phase transitions. An amorphous transition of a nanoparticle can be achieved by its melting and further cooling to room temperature at a 0.2 TK/s rate whereas a crystalline transition, by its heating to 1300–1400 K at a 0.2 TK/s rate followed by cooling. Results of molecular dynamics experiments suggest there is a minimum silicon nanoparticle size for which the development of phase change memory cells becomes theoretically impossible at a given temperature change rate. For a 0.2 TK/s temperature change rate this minimum size is 12.4 nm (number of atoms approx. 5 ∙ 104). https://moem.pensoft.net/article/51788/download/pdf/
collection DOAJ
language English
format Article
sources DOAJ
author Igor V. Talyzin
Vladimir M. Samsonov
spellingShingle Igor V. Talyzin
Vladimir M. Samsonov
Outlooks for development of silicon nanoparticle memory cells
Modern Electronic Materials
author_facet Igor V. Talyzin
Vladimir M. Samsonov
author_sort Igor V. Talyzin
title Outlooks for development of silicon nanoparticle memory cells
title_short Outlooks for development of silicon nanoparticle memory cells
title_full Outlooks for development of silicon nanoparticle memory cells
title_fullStr Outlooks for development of silicon nanoparticle memory cells
title_full_unstemmed Outlooks for development of silicon nanoparticle memory cells
title_sort outlooks for development of silicon nanoparticle memory cells
publisher Pensoft Publishers
series Modern Electronic Materials
issn 2452-1779
publishDate 2019-12-01
description Phase change memory is based on changes in the optical, electrical or other properties of materials during phase transitions, e.g. an amorphous to crystalline transition. Currently existing and potential applications of this memory are primarily based on multicomponent alloys of metals and semiconductors. However single-component nanoparticles including Si ones are also of interest as promising nanosized memory cells. The potential for developing this type of memory cells is confirmed by the fact that the optical absorption index of bulk amorphous silicon is of the same order of magnitude as that of crystalline silicon. Certainly this phenomenon can hardly be implemented with a single nanoparticle the size of which is within light wavelength. Using molecular dynamics and the Stillinger-Weber potential we have studied the regularities of melting and the conditions of crystallization of silicon nanoparticles containing within 105 atoms. We have shown that cooling of nanosized silicon drops at a 0.2 TK/s rate or higher rates causes their amorphous transition whereas single-component nanosized metallic drops crystallize in molecular dynamics experiments even at a 1 TK/s rate. Further heating of amorphous silicon nanoparticles containing above 5 ∙ 104 atoms causes their crystallization in a specific temperature range from 1300 to 1400 K. We have concluded that there is a possibility of developing phase change memory cells on the basis of the above phase transitions. An amorphous transition of a nanoparticle can be achieved by its melting and further cooling to room temperature at a 0.2 TK/s rate whereas a crystalline transition, by its heating to 1300–1400 K at a 0.2 TK/s rate followed by cooling. Results of molecular dynamics experiments suggest there is a minimum silicon nanoparticle size for which the development of phase change memory cells becomes theoretically impossible at a given temperature change rate. For a 0.2 TK/s temperature change rate this minimum size is 12.4 nm (number of atoms approx. 5 ∙ 104).
url https://moem.pensoft.net/article/51788/download/pdf/
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