Giant Hall Resistivity and Magnetoresistance in Cubic Chiral Antiferromagnet EuPtSi

被引:80
作者
Kakihana, Masashi [1 ]
Aoki, Dai [2 ]
Nakamura, Ai [2 ]
Honda, Fuminori [2 ]
Nakashima, Miho [3 ]
Amako, Yasushi [3 ]
Nakamura, Shota [4 ]
Sakakibara, Toshiro [4 ]
Hedo, Masato [5 ]
Nakama, Takao [5 ]
Onuki, Yoshichika [5 ]
机构
[1] Univ Ryukyus, Grad Sch Engn & Sci, Nishihara, Okinawa 9030213, Japan
[2] Tohoku Univ, Inst Mat Res, Oarai, Ibaraki 3111313, Japan
[3] Shinshu Univ, Fac Sci, Matsumoto, Nagano 3908621, Japan
[4] Univ Tokyo, Inst Solid State Phys, Kashiwa, Chiba 2778581, Japan
[5] Univ Ryukyus, Fac Sci, Nishihara, Okinawa 9030213, Japan
关键词
EU-151; MOSSBAUER;
D O I
10.7566/JPSJ.87.023701
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
EuPtSi crystallizes in the cubic chiral structure (P2(1)3, No. 198), which is the same as the non-centrosymmetric space group of MnSi with the skyrmion structure, and orders antiferromagnetically below a Neel temperature T-N = 4.05 K. The magnetization at 2K for the [111] direction indicates two metamagnetic transitions at the magnetic fields H-A1 = 9.2 kOe and H-A2 = 13.8 kOe and saturates above H-c = 26.6 kOe. The present magnetic phase between H-A1 and H-A2 is most likely closed in the (H, T) phase and is observed in a wide temperature range from 3.6 to 0.5 K. In this magnetic phase known as the A-phase, we found giant additional Hall resistivity Delta rho(H)(H) and magnetoresistance Delta rho(H), reaching Delta rho(H)(H) = 0.12 mu Omega.cm and Delta rho(H) = 1.4 mu Omega.cm, respectively. These findings are obtained for H parallel to [111] and [100], but not for H parallel to [110] and [112], revealing an anisotropic behavior in the new material EuPtSi.
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页数:4
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