Field-induced Insulator-Metal Transition in EuTe2

被引:0
作者
Takeuchi, Tetsuya [1 ]
Honda, Fuminori [2 ]
Aoki, Dai [3 ]
Haga, Yoshinori [4 ]
Kida, Takanori [5 ]
Narumi, Yasuo [5 ]
Hagiwara, Masayuki [5 ]
Kindo, Koichi [6 ]
Karube, Kosuke [7 ]
Harima, Hisatomo [8 ]
Onuki, Yoshichika [7 ,9 ]
机构
[1] Osaka Univ, Core Facil Ctr, Cryogen Support Div, Toyonaka, Osaka 5600043, Japan
[2] Kyushu Univ, Cent Inst Radioisotope Sci & Safety, Fukuoka 8190395, Japan
[3] Tohoku Univ, Inst Mat Res, Oarai, Ibaraki 3111313, Japan
[4] JAEA, Adv Sci Res Ctr, Tokai, Ibaraki 3191195, Japan
[5] Osaka Univ, Ctr Adv High Magnet Field Sci, Grad Sch Sci, Toyonaka, Osaka 5600043, Japan
[6] Univ Tokyo, Inst Solid State Phys, Kashiwa, Chiba 2778581, Japan
[7] RIKEN, Ctr Emergent Matter Sci, Wako, Saitama 3510198, Japan
[8] Kobe Univ, Grad Sch Sci, Kobe 6578501, Japan
[9] Tokyo Metropolitan Univ, Dept Phys, Hachioji, Tokyo 1920397, Japan
关键词
SUPERCONDUCTIVITY;
D O I
10.7566/JPSJ.93.044708
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
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 = 11.1 K can be understood in terms of the magnetization processes of the twosublattice 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 mu 0H = 40 T, the insulator-metal transition was found to occur when the magnetization reaches similar to 2 mu B/Eu for both H 11 [110] and [001] at measurement temperatures above 50 K. 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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页数:10
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