Bipartite magnetic parent phases in the iron oxypnictide superconductor
平石 雅俊*; 飯村 壮史*; 小嶋 健児*; 山浦 淳一*; 平賀 晴弘*; 池田 一貴*; Miao, P.*; 石川 喜久*; 鳥居 周輝*; 宮崎 正範*; 山内 一宏*; 幸田 章宏*; 石井 賢司; 吉田 雅洋*; 水木 純一郎*; 門野 良典*; 熊井 玲児*; 神山 崇*; 大友 季哉*; 村上 洋一*; 松石 聡*; 細野 秀雄*
Hiraishi, Masatoshi*; Iimura, Soshi*; Kojima, Kenji*; Yamaura, Junichi*; Hiraka, Haruhiro*; Ikeda, Kazutaka*; Miao, P.*; Ishikawa, Yoshihisa*; Torii, Shuki*; Miyazaki, Masanori*; Yamauchi, Ichihiro*; Koda, Akihiro*; Ishii, Kenji; Yoshida, Masahiro*; Mizuki, Junichiro*; Kadono, Ryosuke*; Kumai, Reiji*; Kamiyama, Takashi*; Otomo, Toshiya*; Murakami, Yoichi*; Matsuishi, Satoru*; Hosono, Hideo*
High-temperature (high-) superconductivity appears as a consequence of the carrier-doping of an undoped parent compound exhibiting antiferromagnetic order; thereby, ground-state properties of the parent compound are closely relevant to the superconducting state. On the basis of the concept, a spin-fluctuation has been addressed as an origin of pairing of the superconducting electrons in cuprates. Whereas, there is growing interest in the pairing mechanism such as an unconventional spin-fluctuation or an advanced orbital-fluctuation due to the characteristic multi-orbital system in iron-pnictides. Here, we report the discovery of an antiferromagnetic order as well as a unique structural transition in electron-overdoped LaFeAsOH (), whereby another parent phase was uncovered, albeit heavily doped. The unprecedented two-dome superconducting phases observed in this material can be interpreted as a consequence of the carrier-doping starting from the original at and advanced at parent phases toward the intermediate region. The bipartite parent phases with distinct physical properties in the second magnetic phase provide us with an interesting example to illustrate the intimate interplay among the magnetic interaction, structural change and orbital degree of freedom in iron-pnictides.