Coexistence of antiferromagnetism and superconductivity in heavy-fermion systems

被引:16
作者
Kitaoka, Y [1 ]
Kawasaki, Y
Mito, T
Kawasaki, S
Zheng, GQ
Ishida, K
Aoki, D
Haga, Y
Settai, R
Onuki, Y
Geibel, C
Steglich, F
机构
[1] Osaka Univ, Grad Sch Engn Sci, Dept Phys Sci, Toyonaka, Osaka 5608531, Japan
[2] Osaka Univ, Grad Sch Sci, Dept Phys, Toyonaka, Osaka 5600043, Japan
[3] Max Planck Inst Chem Phys Solids, D-01187 Dresden, Germany
基金
日本学术振兴会;
关键词
superconductors; crystal structure; superconductivity; magnetic properties; nuclear quadrupole resonance (NQR);
D O I
10.1016/S0022-3697(02)00133-6
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
We report the novel pressure (P)-temperature (T) phase diagrams of antiferromagnetism (AFM) and superconductivity (SC) in CeRhIn5, CeIn3, and CeCu2Si2 revealed by the nuclear quadrupole resonance measurement. In the itinerant helical magnet CeRhIn5, we found that the Neel temperature T-N is reduced at P greater than or equal to 1.23 GPa with an emergent pseudogap behavior. The coexistence of AFM and SC is found in a narrow P range of 1.63-1.75 GPa, followed by the onset of SC with line-node gap over a wide P window 2.1-5 GPa. In CeIn3, the localized magnetic character is robust against the application of pressure up to P similar to 1.9 GPa, beyond which the system evolves into an itinerant regime in which the resistive superconducting phase emerges. We discuss the relationship between the phase diagram and the magnetic fluctuations. In CeCu2Si2, the SC and AFM coexist on a microscopic level once its lattice parameter is expanded. We remark that the underlying marginal AFM state is due to collective magnetic excitations in the superconducting state in CeCu2Si2. An interplay between AFM and SC is discussed on the SO(5) scenario that unifies AFM and SC. We suggest that the SC and AFM in CeCu2Si2 have a common mechanism. (C) 2002 Elsevier Science Ltd. All rights reserved.
引用
收藏
页码:1141 / 1146
页数:6
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