TY - JOUR
T1 - Phase-controllable growth of ultrathin 2D magnetic FeTe crystals
AU - Kang, Lixing
AU - Ye, Chen
AU - Zhao, Xiaoxu
AU - Zhou, Xieyu
AU - Hu, Junxiong
AU - Li, Qiao
AU - Liu, Dan
AU - Das, Chandreyee Manas
AU - Yang, Jiefu
AU - Hu, Dianyi
AU - Chen, Jieqiong
AU - Cao, Xun
AU - Zhang, Yong
AU - Xu, Manzhang
AU - Di, Jun
AU - Tian, Dan
AU - Song, Pin
AU - Kutty, Govindan
AU - Zeng, Qingsheng
AU - Fu, Qundong
AU - Deng, Ya
AU - Zhou, Jiadong
AU - Ariando, Ariando
AU - Miao, Feng
AU - Hong, Guo
AU - Huang, Yizhong
AU - Pennycook, Stephen J.
AU - Yong, Ken Tye
AU - Ji, Wei
AU - Renshaw Wang, Xiao
AU - Liu, Zheng
N1 - Publisher Copyright:
© 2020, The Author(s).
PY - 2020/12/1
Y1 - 2020/12/1
N2 - Two-dimensional (2D) magnets with intrinsic ferromagnetic/antiferromagnetic (FM/AFM) ordering are highly desirable for future spintronic devices. However, the direct growth of their crystals is in its infancy. Here we report a chemical vapor deposition approach to controllably grow layered tetragonal and non-layered hexagonal FeTe nanoplates with their thicknesses down to 3.6 and 2.8 nm, respectively. Moreover, transport measurements reveal these obtained FeTe nanoflakes show a thickness-dependent magnetic transition. Antiferromagnetic tetragonal FeTe with the Néel temperature (TN) gradually decreases from 70 to 45 K as the thickness declines from 32 to 5 nm. And ferromagnetic hexagonal FeTe is accompanied by a drop of the Curie temperature (TC) from 220 K (30 nm) to 170 K (4 nm). Theoretical calculations indicate that the ferromagnetic order in hexagonal FeTe is originated from its concomitant lattice distortion and Stoner instability. This study highlights its potential applications in future spintronic devices.
AB - Two-dimensional (2D) magnets with intrinsic ferromagnetic/antiferromagnetic (FM/AFM) ordering are highly desirable for future spintronic devices. However, the direct growth of their crystals is in its infancy. Here we report a chemical vapor deposition approach to controllably grow layered tetragonal and non-layered hexagonal FeTe nanoplates with their thicknesses down to 3.6 and 2.8 nm, respectively. Moreover, transport measurements reveal these obtained FeTe nanoflakes show a thickness-dependent magnetic transition. Antiferromagnetic tetragonal FeTe with the Néel temperature (TN) gradually decreases from 70 to 45 K as the thickness declines from 32 to 5 nm. And ferromagnetic hexagonal FeTe is accompanied by a drop of the Curie temperature (TC) from 220 K (30 nm) to 170 K (4 nm). Theoretical calculations indicate that the ferromagnetic order in hexagonal FeTe is originated from its concomitant lattice distortion and Stoner instability. This study highlights its potential applications in future spintronic devices.
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U2 - 10.1038/s41467-020-17253-x
DO - 10.1038/s41467-020-17253-x
M3 - Article
C2 - 32709904
AN - SCOPUS:85088381537
SN - 2041-1723
VL - 11
JO - Nature Communications
JF - Nature Communications
IS - 1
M1 - 3729
ER -