TY - JOUR
T1 - Cr-Triggered Local Structural Change in Cr2Ge2Te6 Phase Change Material
AU - Hatayama, Shogo
AU - Shuang, Yi
AU - Fons, Paul
AU - Saito, Yuta
AU - Kolobov, Alexander V.
AU - Kobayashi, Keisuke
AU - Shindo, Satoshi
AU - Ando, Daisuke
AU - Sutou, Yuji
N1 - Funding Information:
This work was supported by KAKENHI (grant nos. 18H02053 and 17 J02967) and Tohoku University Division for Interdisciplinary Advanced Research and Education (DIARE). The EXAFS and HAXPES measurements were performed at beamlines BL01B1 and BL47XU at SPring-8, Japan as parts of proposals of 2017A1383 and 2018A1243, respectively.
Publisher Copyright:
Copyright © 2019 American Chemical Society.
PY - 2019/11/20
Y1 - 2019/11/20
N2 - Cr2Ge2Te6 (CrGT) is a phase change material with higher resistivity in the crystalline phase than in the amorphous phase. CrGT exhibits an ultralow operation energy for amorphization. In this study, the origin of the increased resistance in crystalline CrGT compared to amorphous CrGT and the underlying phase change mechanism were investigated in terms of both local structural change and associated change in electronic state. The density of states at the Fermi level in crystalline CrGT decreased with increasing annealing temperature and became negligible upon annealing at 380 °C. Simultaneously, the Fermi level shifted from the vicinity of the valence band to the band gap center, leading to an increase in resistance. The phase change from amorphous to crystalline CrGT occurred through a metastable crystalline phase with a local structure similar to that of the amorphous phase. Cr nanoclusters were confirmed to exist in both the amorphous and crystalline phases. The presence of Cr nanoclusters induced Cr vacancies in the crystalline phase. These Cr vacancies generated hole carriers, leading to p-type conduction. Photoelectron spectroscopy of the Cr 2s core level clearly indicated a decrease in the fraction of Cr-Cr bonds and an increase in the fraction of Cr-Te bonds in crystalline CrGT upon annealing. Meanwhile, the coordination number of the Cr nanoclusters decreased as the number of Cr-Cr bonds was reduced. Together, these results imply that the origin of the increased resistance in crystalline CrGT is the filling of Cr vacancies by Cr atoms diffusing from Cr nanoclusters.
AB - Cr2Ge2Te6 (CrGT) is a phase change material with higher resistivity in the crystalline phase than in the amorphous phase. CrGT exhibits an ultralow operation energy for amorphization. In this study, the origin of the increased resistance in crystalline CrGT compared to amorphous CrGT and the underlying phase change mechanism were investigated in terms of both local structural change and associated change in electronic state. The density of states at the Fermi level in crystalline CrGT decreased with increasing annealing temperature and became negligible upon annealing at 380 °C. Simultaneously, the Fermi level shifted from the vicinity of the valence band to the band gap center, leading to an increase in resistance. The phase change from amorphous to crystalline CrGT occurred through a metastable crystalline phase with a local structure similar to that of the amorphous phase. Cr nanoclusters were confirmed to exist in both the amorphous and crystalline phases. The presence of Cr nanoclusters induced Cr vacancies in the crystalline phase. These Cr vacancies generated hole carriers, leading to p-type conduction. Photoelectron spectroscopy of the Cr 2s core level clearly indicated a decrease in the fraction of Cr-Cr bonds and an increase in the fraction of Cr-Te bonds in crystalline CrGT upon annealing. Meanwhile, the coordination number of the Cr nanoclusters decreased as the number of Cr-Cr bonds was reduced. Together, these results imply that the origin of the increased resistance in crystalline CrGT is the filling of Cr vacancies by Cr atoms diffusing from Cr nanoclusters.
KW - Cr-Ge-Te
KW - inverse resistance change
KW - local structure
KW - metastable phase
KW - phase change material
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U2 - 10.1021/acsami.9b11535
DO - 10.1021/acsami.9b11535
M3 - Article
C2 - 31647631
AN - SCOPUS:85074687853
SN - 1944-8244
VL - 11
SP - 43320
EP - 43329
JO - ACS Applied Materials and Interfaces
JF - ACS Applied Materials and Interfaces
IS - 46
ER -