Kawasaki S, Mito T, Kawasaki Y, Zheng G-q, Kitaoka Y, Aoki D, Haga Y, Onuki Y
Department of Physical Science, Graduate School of Engineering Science, Osaka University, Toyonaka, Osaka 560-8531, Japan.
Phys Rev Lett. 2003 Sep 26;91(13):137001. doi: 10.1103/PhysRevLett.91.137001. Epub 2003 Sep 23.
We report systematic measurements of ac susceptibility, nuclear-quadrupole-resonance spectrum, and nuclear-spin-lattice-relaxation time (T1) on the pressure (P)-induced heavy-fermion superconductor CeRhIn5. The temperature (T) dependence of 1/T(1) at P=1.6 GPa has revealed that antiferromagnetism (AFM) and superconductivity (SC) coexist microscopically, exhibiting the respective transition at T(N)=2.8 K and T(MF)(c)=0.9 K. It is demonstrated that SC does not yield any trace of gap opening in low-lying excitations below T(onset)(c)=2 K, but T(MF)(c)=0.9 K, followed by a T(1)T=const law. These results point to the unconventional characteristics of SC coexisting with AFM. We highlight that both of the results deserve theoretical work on the gapless nature in the low-lying excitation spectrum due to the coexistence of AFM and SC and the lack of the mean-field regime below T(onset)(c)=2 K.
我们报告了对压力(P)诱导的重费米子超导体CeRhIn5的交流磁化率、核四极共振谱和核自旋晶格弛豫时间(T1)的系统测量。在P = 1.6 GPa时,1/T(1)的温度(T)依赖性表明反铁磁性(AFM)和超导性(SC)在微观上共存,分别在T(N)=2.8 K和T(MF)(c)=0.9 K出现转变。结果表明,在低于T(onset)(c)=2 K的低能激发中,SC没有产生任何能隙打开的迹象,但T(MF)(c)=0.9 K,随后遵循T(1)T = const定律。这些结果表明与AFM共存的SC具有非常规特性。我们强调,由于AFM和SC的共存以及在低于T(onset)(c)=2 K时缺乏平均场区域,这两个结果都值得对低能激发谱中的无隙性质进行理论研究。