Sung H H, Wu H H, Syu K J, Lee W H, Chen Y Y
Department of Physics, National Chung Cheng University, Ming-Hsiung, Chia-Yi 621, Taiwan, Republic of China.
J Phys Condens Matter. 2009 Apr 29;21(17):176004. doi: 10.1088/0953-8984/21/17/176004. Epub 2009 Mar 30.
We find that Ce(Ni(0.25)In(1.75)) crystallizes in the hexagonal AlB(2)-type structure with lattice parameters a = 0.4850(5) nm and c = 0.3908(5) nm. Magnetic susceptibility, electrical resistivity and low-temperature specific heat data reveal that the bulk phase transition at 3.7 ± 0.2 K in Ce(Ni(0.25)In(1.75)) is to an antiferromagnetic state. The magnetic contribution to the resistivity ρ(mag) of Ce(Ni(0.25)In(1.75)) increases as ln(T) when temperature is lowered from room temperature and reaches a plateau at 9 K, followed by a rapid decrease around 4 K. These results associated with a reduction of the Ce magnetic moment and of the magnetic entropy at T(N) suggest that Ce(Ni(0.25)In(1.75)) could be a Kondo antiferromagnet. The Kondo temperature is estimated to be of order 6 K.
我们发现Ce(Ni(0.25)In(1.75))以六方AlB₂型结构结晶,晶格参数a = 0.4850(5)纳米,c = 0.3908(5)纳米。磁化率、电阻率和低温比热数据表明,Ce(Ni(0.25)In(1.75))在3.7±0.2 K时的体相转变为反铁磁态。当温度从室温降低时,Ce(Ni(0.25)In(1.75))的电阻率磁贡献ρ(mag)随ln(T)增加,并在9 K时达到平台,随后在4 K左右迅速下降。这些与T(N)时Ce磁矩和磁熵降低相关的结果表明,Ce(Ni(0.25)In(1.75))可能是一种近藤反铁磁体。近藤温度估计约为6 K。