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Department of Physics and Chemistry
Novel Quantum Materials Laboratory
1. Journal Articles
Metal-insulator transition and doping-induced phase change in Ge 2 Sb 2 Se 5 x Te 5 - 5 x
Xu, Zhenyang
;
Park, Keeseong
;
Schneeloch, John A.
;
Louca, Despina
Department of Physics and Chemistry
Novel Quantum Materials Laboratory
1. Journal Articles
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Title
Metal-insulator transition and doping-induced phase change in Ge 2 Sb 2 Se 5 x Te 5 - 5 x
DGIST Authors
Park, Keeseong
Issued Date
2020-11
Citation
Xu, Zhenyang. (2020-11). Metal-insulator transition and doping-induced phase change in Ge 2 Sb 2 Se 5 x Te 5 - 5 x. doi: 10.1063/5.0030956
Type
Article
Article Type
Article
Author Keywords
Hexagonal phase
;
Induced phase change
;
Liquid nitrogen quenched
;
Metal-to-insulator transitions
;
Optical characteristics
;
Orders of magnitude
;
Metal insulator transition
;
Activation energy
;
Antimony
;
Antimony compounds
;
Doping (additives)
;
Germanium
;
Germanium compounds
;
Ground state
;
Liquefied gases
;
Metal insulator boundaries
;
Nanocrystalline materials
;
Phase change materials
;
Salt deposits
;
Selenium
;
Semiconductor insulator boundaries
;
Tellurium
;
Amorphous and crystalline phasis
;
Hexagonal crystals
Keywords
KINETICS
;
CRYSTALLIZATION
;
DIFFRACTION
;
FILMS
ISSN
0003-6951
Abstract
Ge2Sb2Te5 (GST-225), a phase change material (PCM) with vast differences in the electrical and optical characteristics between its amorphous and crystalline phases, is revisited to explore its properties with Se doping. GST crystallizes in a layered hexagonal ground state, while the precursor to the amorphous state is a distorted rock salt like structure with vacancies at the Ge/Sb sites. Upon doping, liquid nitrogen quenched Ge 2 Sb 2 Se 5 x Te 5 - 5 x (GSST-225) exhibits a direct hexagonal-to-amorphous phase change above x > 0.8, whereas the rock salt like structure appears as a second phase with a volume fraction that does not change as a function of the doping. The phase change is accompanied by a metal-to-insulator transition (MIT), with a several orders of magnitude increase in the resistivity on approaching the amorphous state. A similar MIT is observed even without the phase change in hexagonal crystals with doping levels above x > 0.8. On warming amorphous GSST (x = 0.9) above room temperature, a reversal to the hexagonal phase occurs with a re-crystallization onset temperature (Tc) above 300 °C, much higher than the Tc (∼ 170 °C) of amorphous GST and an activation energy of 1.47 eV, which is comparable to good glass formers. © 2020 Author(s).
URI
http://hdl.handle.net/20.500.11750/12790
DOI
10.1063/5.0030956
Publisher
American Institute of Physics Inc.
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