Spin density wave in quasi-one-dimensional organic conductors

被引:0
|
作者
Nomura, K [1 ]
Matsunaga, N
Ishikawa, A
Kotani, H
Yamashita, K
Sasaki, T
Hanajiri, T
Yamada, J
Nakatsuji, S
Anzai, H
Nakamura, T
Takahashi, T
Saito, G
机构
[1] Hokkaido Univ, Div Phys, Sapporo, Hokkaido 0600810, Japan
[2] Tohoku Univ, IMR, Sendai, Miyagi 9808577, Japan
[3] Himeji Inst Technol, Dept Mat Sci, Himeji, Hyogo 6781297, Japan
[4] Inst Mol Sci, Okazaki, Aichi 4448585, Japan
[5] Gakushuin Univ, Dept Phys, Tokyo 1718588, Japan
[6] Kyoto Univ, Dept Chem, Kyoto 6068502, Japan
来源
PHYSICA STATUS SOLIDI B-BASIC RESEARCH | 2001年 / 223卷 / 02期
关键词
D O I
10.1002/1521-3951(200101)223:2<449::AID-PSSB449>3.0.CO;2-A
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
The incommensurate spin density wave (SDW) phases in (TMTSF)(2)PF6 and (TMTTF)(2)Br were investigated by transport measurements under pressure and in magnetic field parallel to the c*-axis. For the SDW phase of (TMTSF)(2)PF6 slightly suppressed by the pressure. the SDW transition temperature T-SDW increases with the applied magnetic field. The field dependence of T-SDW is de scribed by a quadratic behavior and the coefficient of the quadratic term increases with increasing pressure. For the incommensurate SDW phase of (TMTTF)(2)Br stabilized under the pressure above 0.5 GPa, the SDW transition shows similar behavior as in the case of (TMTSF)(2)PF6 with increasing magnetic field. These results are consistent with the prediction of the mean field theory based on the nesting of the Fermi surface. The incommensurate SDW phases in both (TMTSF)(2)PF6 and (TMTTF)(2)Br are understood in a common pressure axis with Laking the reduction of the coupling constant by the pressure into account.
引用
收藏
页码:449 / 458
页数:10
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