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The Effect of Carbon Doping on the Crystal Structure and Electrical Properties of Sb(2)Te(3)

As a new generation of non-volatile memory, phase change random access memory (PCRAM) has the potential to fill the hierarchical gap between DRAM and NAND FLASH in computer storage. Sb(2)Te(3), one of the candidate materials for high-speed PCRAM, has high crystallization speed and poor thermal stabi...

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Autores principales: Zhang, Jie, Rong, Ningning, Xu, Peng, Xiao, Yuchen, Lu, Aijiang, Song, Wenxiong, Song, Sannian, Song, Zhitang, Liang, Yongcheng, Wu, Liangcai
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9959287/
https://www.ncbi.nlm.nih.gov/pubmed/36839039
http://dx.doi.org/10.3390/nano13040671
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author Zhang, Jie
Rong, Ningning
Xu, Peng
Xiao, Yuchen
Lu, Aijiang
Song, Wenxiong
Song, Sannian
Song, Zhitang
Liang, Yongcheng
Wu, Liangcai
author_facet Zhang, Jie
Rong, Ningning
Xu, Peng
Xiao, Yuchen
Lu, Aijiang
Song, Wenxiong
Song, Sannian
Song, Zhitang
Liang, Yongcheng
Wu, Liangcai
author_sort Zhang, Jie
collection PubMed
description As a new generation of non-volatile memory, phase change random access memory (PCRAM) has the potential to fill the hierarchical gap between DRAM and NAND FLASH in computer storage. Sb(2)Te(3), one of the candidate materials for high-speed PCRAM, has high crystallization speed and poor thermal stability. In this work, we investigated the effect of carbon doping on Sb(2)Te(3). It was found that the FCC phase of C-doped Sb(2)Te(3) appeared at 200 °C and began to transform into the HEX phase at 25 °C, which is different from the previous reports where no FCC phase was observed in C-Sb(2)Te(3). Based on the experimental observation and first-principles density functional theory calculation, it is found that the formation energy of FCC-Sb(2)Te(3) structure decreases gradually with the increase in C doping concentration. Moreover, doped C atoms tend to form C molecular clusters in sp(2) hybridization at the grain boundary of Sb(2)Te(3), which is similar to the layered structure of graphite. And after doping C atoms, the thermal stability of Sb(2)Te(3) is improved. We have fabricated the PCRAM device cell array of a C-Sb(2)Te(3) alloy, which has an operating speed of 5 ns, a high thermal stability (10-year data retention temperature 138.1 °C), a low device power consumption (0.57 pJ), a continuously adjustable resistance value, and a very low resistance drift coefficient.
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spelling pubmed-99592872023-02-26 The Effect of Carbon Doping on the Crystal Structure and Electrical Properties of Sb(2)Te(3) Zhang, Jie Rong, Ningning Xu, Peng Xiao, Yuchen Lu, Aijiang Song, Wenxiong Song, Sannian Song, Zhitang Liang, Yongcheng Wu, Liangcai Nanomaterials (Basel) Article As a new generation of non-volatile memory, phase change random access memory (PCRAM) has the potential to fill the hierarchical gap between DRAM and NAND FLASH in computer storage. Sb(2)Te(3), one of the candidate materials for high-speed PCRAM, has high crystallization speed and poor thermal stability. In this work, we investigated the effect of carbon doping on Sb(2)Te(3). It was found that the FCC phase of C-doped Sb(2)Te(3) appeared at 200 °C and began to transform into the HEX phase at 25 °C, which is different from the previous reports where no FCC phase was observed in C-Sb(2)Te(3). Based on the experimental observation and first-principles density functional theory calculation, it is found that the formation energy of FCC-Sb(2)Te(3) structure decreases gradually with the increase in C doping concentration. Moreover, doped C atoms tend to form C molecular clusters in sp(2) hybridization at the grain boundary of Sb(2)Te(3), which is similar to the layered structure of graphite. And after doping C atoms, the thermal stability of Sb(2)Te(3) is improved. We have fabricated the PCRAM device cell array of a C-Sb(2)Te(3) alloy, which has an operating speed of 5 ns, a high thermal stability (10-year data retention temperature 138.1 °C), a low device power consumption (0.57 pJ), a continuously adjustable resistance value, and a very low resistance drift coefficient. MDPI 2023-02-09 /pmc/articles/PMC9959287/ /pubmed/36839039 http://dx.doi.org/10.3390/nano13040671 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Zhang, Jie
Rong, Ningning
Xu, Peng
Xiao, Yuchen
Lu, Aijiang
Song, Wenxiong
Song, Sannian
Song, Zhitang
Liang, Yongcheng
Wu, Liangcai
The Effect of Carbon Doping on the Crystal Structure and Electrical Properties of Sb(2)Te(3)
title The Effect of Carbon Doping on the Crystal Structure and Electrical Properties of Sb(2)Te(3)
title_full The Effect of Carbon Doping on the Crystal Structure and Electrical Properties of Sb(2)Te(3)
title_fullStr The Effect of Carbon Doping on the Crystal Structure and Electrical Properties of Sb(2)Te(3)
title_full_unstemmed The Effect of Carbon Doping on the Crystal Structure and Electrical Properties of Sb(2)Te(3)
title_short The Effect of Carbon Doping on the Crystal Structure and Electrical Properties of Sb(2)Te(3)
title_sort effect of carbon doping on the crystal structure and electrical properties of sb(2)te(3)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9959287/
https://www.ncbi.nlm.nih.gov/pubmed/36839039
http://dx.doi.org/10.3390/nano13040671
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