TY - JOUR
T1 - Field-induced Insulator–Metal Transition in EuTe2
AU - Takeuchi, Tetsuya
AU - Honda, Fuminori
AU - Aoki, Dai
AU - Haga, Yoshinori
AU - Kida, Takanori
AU - Narumi, Yasuo
AU - Hagiwara, Masayuki
AU - Kindo, Koichi
AU - Karube, Kosuke
AU - Harima, Hisatomo
AU - Ōnuki, Yoshichika
N1 - Publisher Copyright:
©2024 The Physical Society of Japan.
PY - 2024/4
Y1 - 2024/4
N2 - We studied in detail the electrical and magnetic properties of the Eu-divalent antiferromagnet EuTe2 with a tetragonal crystal structure using single crystals grown by the Te self-flux method. The observed anisotropic magnetization curves in the antiferromagnetic state below TN = 11.1K can be understood in terms of the magnetization processes of the two-sublattice model of an antiferromagnet with uniaxial magnetic anisotropy. A characteristic feature of this compound is that it becomes an insulator with decreasing temperature at zero magnetic field, but changes to a metal with a relatively low number of carriers in magnetic fields. From the results of magnetization, magnetoresistance, and Hall resistivity measurements in magnetic fields up to μ0H = 40T, the insulator–metal transition was found to occur when the magnetization reaches ∼2μB=Eu for both H k ½110] and [001] at measurement temperatures above 50K. Energy band calculations revealed that only the up-spin band, which is mainly composed of Te-5p electrons, crosses the Fermi level in the ferromagnetic state, although the energy band possesses a band gap in the paramagnetic and antiferromagnetic states.
AB - We studied in detail the electrical and magnetic properties of the Eu-divalent antiferromagnet EuTe2 with a tetragonal crystal structure using single crystals grown by the Te self-flux method. The observed anisotropic magnetization curves in the antiferromagnetic state below TN = 11.1K can be understood in terms of the magnetization processes of the two-sublattice model of an antiferromagnet with uniaxial magnetic anisotropy. A characteristic feature of this compound is that it becomes an insulator with decreasing temperature at zero magnetic field, but changes to a metal with a relatively low number of carriers in magnetic fields. From the results of magnetization, magnetoresistance, and Hall resistivity measurements in magnetic fields up to μ0H = 40T, the insulator–metal transition was found to occur when the magnetization reaches ∼2μB=Eu for both H k ½110] and [001] at measurement temperatures above 50K. Energy band calculations revealed that only the up-spin band, which is mainly composed of Te-5p electrons, crosses the Fermi level in the ferromagnetic state, although the energy band possesses a band gap in the paramagnetic and antiferromagnetic states.
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U2 - 10.7566/JPSJ.93.044708
DO - 10.7566/JPSJ.93.044708
M3 - Article
AN - SCOPUS:85189306334
SN - 0031-9015
VL - 93
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 4
M1 - 044708
ER -