Sun J P, Wang Z-C, Liu Z Y, Xu S X, Eto T, Sui Y, Wang B S, Uwatoko Y, Cao G-H, Cheng J-G
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China. School of Physical Sciences, University of Chinese Academy of Sciences, Beijing 100190, People's Republic of China.
J Phys Condens Matter. 2019 Jan 30;31(4):044001. doi: 10.1088/1361-648X/aaf0b9.
RbGdFeAsO is a newly discovered self-hole-doped stoichiometric superconductor, which has a hybrid structure with separated double FeAs layers and exhibits a high superconducting transition temperature T = 35 K. Here, we report the effect of pressure (P) on its T and normal-state transport properties by measuring the temperature dependence of resistivity ρ(T) under various pressures up to 14 GPa with a cubic anvil cell apparatus. We found that the T is suppressed monotonically to ca. 12.5 K upon increasing pressure to 14 GPa with a slope change of T (P) at around 4 GPa. In addition, the low-temperature normal-state ρ(T), which is proportional to T , also evolves gradually from a non-Fermi-liquid with n = 1 at ambient pressure to a Fermi liquid with n = 2 at P ⩾ 4 GPa. Accompanying with the non-Fermi-liquid to Fermi-liquid crossover, the quadratic temperature coefficient of resistivity, which reflects the effective mass of charge carriers, also experiences a significant reduction as commonly observed in the vicinity of a magnetic quantum critical point (QCP). Our results indicate that the stoichiometric RbGdFeAsO at ambient pressure might be located near a QCP such that the enhanced critical spin fluctuations lead to high-T superconductivity. The application of pressure should broaden the electronic bandwidth and weaken the spin fluctuations, and then restore a Fermi-liquid ground state with lower T .
RbGdFeAsO是一种新发现的自空穴掺杂化学计量超导体,它具有分离的双FeAs层的混合结构,并且表现出较高的超导转变温度(T_c = 35K)。在此,我们通过使用立方砧室装置测量高达14GPa的各种压力下电阻率(\rho(T))的温度依赖性,报告压力(P)对其(T_c)和正常态输运性质的影响。我们发现,随着压力增加到14GPa,(T_c)单调下降至约12.5K,在约4GPa处(T_c(P))有斜率变化。此外,与(T^2)成正比的低温正常态(\rho(T))也逐渐从常压下(n = 1)的非费米液体演变为(P\geqslant4GPa)时(n = 2)的费米液体。伴随着从非费米液体到费米液体的转变,反映电荷载流子有效质量的电阻率二次温度系数也如在磁量子临界点(QCP)附近通常观察到的那样经历显著降低。我们的结果表明,常压下的化学计量RbGdFeAsO可能位于QCP附近,使得增强的临界自旋涨落导致高温超导。压力的施加应拓宽电子带宽并减弱自旋涨落,然后恢复具有较低(T_c)的费米液体基态。