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In Situ Temperature-Dependent Transmission Electron Microscopy Studies of Psedobinary mGeTe center dot Bi2Te3 (m=3-8) Nanowires and First-Principles Calculations

Authors
Jung, Chan SuKim, Han SungIm, Hyung SoonPark, KidongPark, JeungheeAhn, Jae-PyoungYoo, Seung JoKim, Jin-GyuKim, Jae NyeongShim, Ji Hoon
Issue Date
Jun-2015
Publisher
AMER CHEMICAL SOC
Keywords
Phase-change materials; GeTe center dot Bi2Te3; nanowires; superlattice; electrical conductivity
Citation
NANO LETTERS, v.15, no.6, pp.3923 - 3930
Indexed
SCIE
SCOPUS
Journal Title
NANO LETTERS
Volume
15
Number
6
Start Page
3923
End Page
3930
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/93379
DOI
10.1021/acs.nanolett.5b00755
ISSN
1530-6984
Abstract
Phase-change nanowires (NWs) have emerged as critical materials for fast-switching nonvolatile memory devices. In this study, we synthesized a series of mGeTe.Bi2Te3 (GBT) pseudobinary alloy NWsGe(3)Bi(2)Te(6) (m = 3), Ge4Bi2Te7 (m = 4), Ge5Bi2Te8 (m = 5), Ge6Bi2Te9 (m = 6), and Ge8Bi2Te11 (m = 8)and investigated their composition-dependent thermal stabilities and electrical properties. As m decreases, the phase of the NWs evolves from the cubic (C) to the hexagonal (H) phase, which produces unique superlattice structures that consist of periodic 2.2-3.8 nm slabs for m = 3-8. In situ temperature-dependent transmission electron microscopy reveals the higher thermal stability of the compositions with lower m values, and a phase transition from the H phase into the single-crystalline C phase at high temperatures (400 degrees C). First-principles calculations, performed for the superlattice structures (m = 1-8) of GBT and mGeTe.Sb2Te3 (GST), show an increasing stability of the H phase (versus the C phase) with decreasing m; the difference in stability being more marked for GBT than for GST. The calculations explain remarkably the phase evolution of the GBT and GST NWs as well as the composition-dependent thermal stabilities. Measurement of the current-voltage curves for individual GBT NWs shows that the resistivity is in the range 3-25 mO.cm, and the resistivity of the H phase is lower than that of the C phase, which has been supported by the calculations.
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