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Phase-Change-Memory Process at the Limit: A Proposal for Utilizing Monolayer Sb2Te3.


ABSTRACT: One central task of developing nonvolatile phase change memory (PCM) is to improve its scalability for high-density data integration. In this work, by first-principles molecular dynamics, to date the thinnest PCM material possible (0.8 nm), namely, a monolayer Sb2Te3, is proposed. Importantly, its SET (crystallization) process is a fast one-step transition from amorphous to hexagonal phase without the usual intermediate cubic phase. An increased spatial localization of electrons due to geometrical confinement is found to be beneficial for keeping the data nonvolatile in the amorphous phase at the 2D limit. The substrate and superstrate can be utilized to control the phase change behavior: e.g., with passivated SiO2 (001) surfaces or hexagonal Boron Nitride, the monolayer Sb2Te3 can reach SET recrystallization in 0.54 ns or even as fast as 0.12 ns, but with unpassivated SiO2 (001), this would not be possible. Besides, working with small volume PCM materials is also a natural way to lower power consumption. Therefore, the proposed PCM working process at the 2D limit will be an important potential strategy of scaling the current PCM materials for ultrahigh-density data storage.

SUBMITTER: Wang XP 

PROVIDER: S-EPMC8261487 | biostudies-literature | 2021 Jul

REPOSITORIES: biostudies-literature

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Phase-Change-Memory Process at the Limit: A Proposal for Utilizing Monolayer Sb<sub>2</sub>Te<sub>3</sub>.

Wang Xue-Peng XP   Li Xian-Bin XB   Chen Nian-Ke NK   Chen Bin B   Rao Feng F   Zhang Shengbai S  

Advanced science (Weinheim, Baden-Wurttemberg, Germany) 20210514 13


One central task of developing nonvolatile phase change memory (PCM) is to improve its scalability for high-density data integration. In this work, by first-principles molecular dynamics, to date the thinnest PCM material possible (0.8 nm), namely, a monolayer Sb<sub>2</sub>Te<sub>3</sub>, is proposed. Importantly, its SET (crystallization) process is a fast one-step transition from amorphous to hexagonal phase without the usual intermediate cubic phase. An increased spatial localization of elec  ...[more]

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