Hefei National Laboratory for Physical Sciences at Microscale, Department of Physics, University of Science and Technology of China, Hefei 230026, People's Republic of China.
J Phys Condens Matter. 2010 Jul 14;22(27):275701. doi: 10.1088/0953-8984/22/27/275701. Epub 2010 Jun 17.
The field and temperature dependencies of the spin structures in the normal states of La(1.6-x)Nd(0.4)Sr(x)CuO(4) (x = 0.10, 0.12, and 0.15) single crystals have been studied by measuring the magnetoresistance and susceptibility. A negative magnetoresistance appears just below the spin-ordering temperature for the magnetic fields parallel to the CuO(2) plane, which can be attributed to the spin-flop transition of the special spin structure in the normal state of the system. The anisotropic variations of susceptibilities with temperature for all the three specimens can be described in the framework of the crystal-field theory. The well fitted broad peaks of the in-plane susceptibilities χ(ab) for the specimens suggest that the susceptibilities are dominated by Nd(3+), and thus the spin reorientation of Cu(2+) in the CuO(2) plane can not be observed from the study of the susceptibility.
通过测量电阻磁强率和磁化率,我们研究了 La(1.6-x)Nd(0.4)Sr(x)CuO(4)(x = 0.10、0.12 和 0.15)单晶体正常态中自旋结构的场和温度依赖性。在磁场平行于 CuO(2) 平面时,低于自旋有序温度会出现负电阻磁强率,这归因于系统正常态中特殊自旋结构的自旋倾斜跃迁。对于所有三个样本,磁化率随温度的各向异性变化都可以用晶场理论来描述。样本的面内磁化率 χ(ab) 的良好拟合宽峰表明,磁化率主要由 Nd(3+) 主导,因此,在磁化率研究中无法观察到 Cu(2+) 在 CuO(2) 平面中的自旋重定向。