Magnetic structure of a non-centrosymmetric CePtSi3

被引:5
|
作者
Ueta, D. [1 ]
Yoshida, M. [1 ]
Ikeda, Y. [2 ]
Liu, Y. [3 ]
Hong, T. [3 ]
Masuda, T. [1 ]
Yoshizawa, H. [1 ]
机构
[1] Univ Tokyo, Inst Solid State Phys, Kashiwa, Chiba 2778581, Japan
[2] Tohoku Univ, Inst Mat Res, Sendai, Miyagi 9808577, Japan
[3] Oak Ridge Natl Lab, Neutron Scattering Div, Oak Ridge, TN 37831 USA
来源
AIP ADVANCES | 2018年 / 8卷 / 11期
基金
美国能源部;
关键词
D O I
10.1063/1.5042736
中图分类号
TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
Neutron diffraction experiments have been performed on single crystalline samples of CePtSi3. We found that the incommensurate magnetic propagation vector tau(1) = (+/- 0.283, 0, 0) in the phase I (2.2 similar to 4.8 K) switches to the commensurate vectors tau(2) = (+/- 0.25, 0, 0) and tau(3) = (+/- 0.25, 0, +/- 1) in the phase III (similar to 2.8 K) at zero field. Although the magnetic structure of CePtSi3 in the phase I is a spin density wave similar to those in CeRhSi3, CeIrSi3, and CePdSi3, the magnetic structure in the phase III is commensurate unlike other CeTSi3 (T = Rh, Ir, Pd) compounds. (c) 2018 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license
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页数:5
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