Ishida Junichi, Iimura Soshi, Matsuishi Satoru, Hosono And Hideo
Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan.
J Phys Condens Matter. 2014 Oct 29;26(43):435702. doi: 10.1088/0953-8984/26/43/435702. Epub 2014 Oct 9.
Hydrogen-doped LaFeAsO(1-x)H(x) system has a unique 2-dome structure. The effects of Zn impurities on the first and second superconducting domes in LaFe(1-y)Zn(y)AsO(1-x)H(x) (x = 0.10 for the first superconducting phase (SC1) and 0.35 for the second superconducting phase (SC2)) are examined by electrical resistivity, Hall effect and magnetization measurements. Substitution with Zn strongly suppresses the critical temperature (Tc) and behaves as a nonmagnetic impurity. The suppression rates are: 17(4) K/% (SC1) and 6.9(5) K/% (SC2). It was considered that Zn impurities induced Anderson localization, which triggered the disappearance of the superconductivity, but no decisive conclusions on the dominant pairing symmetry for each dome were obtained.
氢掺杂的LaFeAsO(1 - x)H(x)体系具有独特的双穹顶结构。通过电阻率、霍尔效应和磁化测量,研究了Zn杂质对LaFe(1 - y)Zn(y)AsO(1 - x)H(x)(对于第一超导相(SC1),x = 0.10;对于第二超导相(SC2),x = 0.35)中第一和第二超导穹顶的影响。用Zn替代会强烈抑制临界温度(Tc),并且表现为非磁性杂质。抑制率分别为:17(4) K/%(SC1)和6.9(5) K/%(SC2)。曾认为Zn杂质诱导了安德森局域化,从而导致超导性消失,但对于每个穹顶的主导配对对称性未得出决定性结论。