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

被引:12
|
作者
Jung, Chan Su [1 ]
Kim, Han Sung [1 ,2 ]
Im, Hyung Soon [1 ]
Park, Kidong [1 ]
Park, Jeunghee [1 ]
Ahn, Jae-Pyoung [2 ]
Yoo, Seung Jo [3 ]
Kim, Jin-Gyu [3 ]
Kim, Jae Nyeong [4 ]
Shim, Ji Hoon [4 ,5 ,6 ]
机构
[1] Korea Univ, Dept Chem, Jochiwon 339700, South Korea
[2] Korea Inst Sci & Technol, Adv Anal Ctr, Seoul 136791, South Korea
[3] Korea Basic Sci Inst, Nanobio Electron Microscopy Res Grp, Taejon 305806, South Korea
[4] Pohang Univ Sci & Technol, Dept Chem, Pohang 790784, South Korea
[5] Pohang Univ Sci & Technol, Dept Phys, Pohang 790784, South Korea
[6] Pohang Univ Sci & Technol, Div Adv Nucl Engn, Pohang 790784, South Korea
关键词
Phase-change materials; GeTe center dot Bi2Te3; nanowires; superlattice; electrical conductivity; PHASE-CHANGE MATERIALS; CHEMICAL-VAPOR-DEPOSITION; CHANGE MEMORY; THIN-FILMS; SPEED; GE2SB2TE5; CONDUCTIVITY; DIFFRACTION; TRANSITIONS; NONVOLATILE;
D O I
10.1021/acs.nanolett.5b00755
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
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.
引用
收藏
页码:3923 / 3930
页数:8
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