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Large-moment antiferromagnetic order in overdoped high-Tc superconductor 154SmFeAsO1-x D x.
Iimura, Soshi; Okanishi, Hiroshi; Matsuishi, Satoru; Hiraka, Haruhiro; Honda, Takashi; Ikeda, Kazutaka; Hansen, Thomas C; Otomo, Toshiya; Hosono, Hideo.
Afiliação
  • Iimura S; Laboratory for Materials and Structures, Tokyo Institute of Technology, Yokohama 226-8503, Japan.
  • Okanishi H; Laboratory for Materials and Structures, Tokyo Institute of Technology, Yokohama 226-8503, Japan.
  • Matsuishi S; Research Center for Element Strategy, Tokyo Institute of Technology, Yokohama 226-8503, Japan.
  • Hiraka H; Graduate School of Science and Engineering, Ibaraki University, Mito 310-8512, Japan.
  • Honda T; Institute of Materials Structure Science, High Energy Accelerator Research Organization, Tsukuba 305-0801, Japan.
  • Ikeda K; Institute of Materials Structure Science, High Energy Accelerator Research Organization, Tsukuba 305-0801, Japan.
  • Hansen TC; Institut Laue-Langevin, 38042 Grenoble Cedex 9, France.
  • Otomo T; Institute of Materials Structure Science, High Energy Accelerator Research Organization, Tsukuba 305-0801, Japan.
  • Hosono H; Department of Materials Structure Science, The Graduate University for Advanced Studies, Tsukuba 305-0801, Japan.
Proc Natl Acad Sci U S A ; 114(22): E4354-E4359, 2017 05 30.
Article em En | MEDLINE | ID: mdl-28507123
ABSTRACT
In iron-based superconductors, high critical temperature (Tc) superconductivity over 50 K has only been accomplished in electron-doped hREFeAsO (hRE is heavy rare earth (RE) element). Although hREFeAsO has the highest bulk Tc (58 K), progress in understanding its physical properties has been relatively slow due to difficulties in achieving high-concentration electron doping and carrying out neutron experiments. Here, we present a systematic neutron powder diffraction study of 154SmFeAsO1-x D x , and the discovery of a long-range antiferromagnetic ordering with x ≥ 0.56 (AFM2) accompanying a structural transition from tetragonal to orthorhombic. Surprisingly, the Fe magnetic moment in AFM2 reaches a magnitude of 2.73 µB/Fe, which is the largest in all nondoped iron pnictides and chalcogenides. Theoretical calculations suggest that the AFM2 phase originates in kinetic frustration of the Fe-3dxy orbital, in which the nearest-neighbor hopping parameter becomes zero. The unique phase diagram, i.e., highest-Tc superconducting phase adjacent to the strongly correlated phase in electron-overdoped regime, yields important clues to the unconventional origins of superconductivity.
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Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2017 Tipo de documento: Article