Large-moment antiferromagnetic order in overdoped high-T c superconductor 154SmFeAsO1−xDₓ
In iron-based superconductors, high critical temperature (T c) 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 T c (58 K), progress in understanding its physical properties has been relat...
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Veröffentlicht in: | Proceedings of the National Academy of Sciences - PNAS 2017-05, Vol.114 (22), p.E4354-E4359 |
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creator | Iimura, Soshi Okanishi, Hiroshi Matsuishi, Satoru Hiraka, Haruhiro Honda, Takashi Ikeda, Kazutaka Hansen, Thomas C. Otomo, Toshiya Hosono, Hideo |
description | In iron-based superconductors, high critical temperature (T
c) 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 T
c (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−xDₓ, 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-T
c superconducting phase adjacent to the strongly correlated phase in electron-overdoped regime, yields important clues to the unconventional origins of superconductivity. |
format | Article |
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c) 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 T
c (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−xDₓ, 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-T
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c) 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 T
c (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−xDₓ, 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-T
c superconducting phase adjacent to the strongly correlated phase in electron-overdoped regime, yields important clues to the unconventional origins of superconductivity.</description><issn>0027-8424</issn><issn>1091-6490</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNqFy7sKwjAUgOEgCtbLIwh5gUDaptqO4gUHwcGuUkJ7bFNMUk6q6OrkrG_ok-jg7vQPH3-HeD5PfDYVCe8Sj_NgxmIRiD4ZOFdzzpMo5h45bCWWwLTVYFoqTauOgGi1LA20KqcWC0CqDLUXwMI2UNBKlRVLaU7duQHMrSnOeWuR-pHY6zXM3c5_P57X5fv-GpHeUZ4cjH8dksl6lS42rHbfI2tQaYm3LJiKOAyTIPznH2I6Qgo</recordid><startdate>20170530</startdate><enddate>20170530</enddate><creator>Iimura, Soshi</creator><creator>Okanishi, Hiroshi</creator><creator>Matsuishi, Satoru</creator><creator>Hiraka, Haruhiro</creator><creator>Honda, Takashi</creator><creator>Ikeda, Kazutaka</creator><creator>Hansen, Thomas C.</creator><creator>Otomo, Toshiya</creator><creator>Hosono, Hideo</creator><general>National Academy of Sciences</general><scope/></search><sort><creationdate>20170530</creationdate><title>Large-moment antiferromagnetic order in overdoped high-T c superconductor 154SmFeAsO1−xDₓ</title><author>Iimura, Soshi ; Okanishi, Hiroshi ; Matsuishi, Satoru ; Hiraka, Haruhiro ; Honda, Takashi ; Ikeda, Kazutaka ; Hansen, Thomas C. ; Otomo, Toshiya ; Hosono, Hideo</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-jstor_primary_264833923</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Iimura, Soshi</creatorcontrib><creatorcontrib>Okanishi, Hiroshi</creatorcontrib><creatorcontrib>Matsuishi, Satoru</creatorcontrib><creatorcontrib>Hiraka, Haruhiro</creatorcontrib><creatorcontrib>Honda, Takashi</creatorcontrib><creatorcontrib>Ikeda, Kazutaka</creatorcontrib><creatorcontrib>Hansen, Thomas C.</creatorcontrib><creatorcontrib>Otomo, Toshiya</creatorcontrib><creatorcontrib>Hosono, Hideo</creatorcontrib><jtitle>Proceedings of the National Academy of Sciences - PNAS</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Iimura, Soshi</au><au>Okanishi, Hiroshi</au><au>Matsuishi, Satoru</au><au>Hiraka, Haruhiro</au><au>Honda, Takashi</au><au>Ikeda, Kazutaka</au><au>Hansen, Thomas C.</au><au>Otomo, Toshiya</au><au>Hosono, Hideo</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Large-moment antiferromagnetic order in overdoped high-T c superconductor 154SmFeAsO1−xDₓ</atitle><jtitle>Proceedings of the National Academy of Sciences - PNAS</jtitle><date>2017-05-30</date><risdate>2017</risdate><volume>114</volume><issue>22</issue><spage>E4354</spage><epage>E4359</epage><pages>E4354-E4359</pages><issn>0027-8424</issn><eissn>1091-6490</eissn><abstract>In iron-based superconductors, high critical temperature (T
c) 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 T
c (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−xDₓ, 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-T
c superconducting phase adjacent to the strongly correlated phase in electron-overdoped regime, yields important clues to the unconventional origins of superconductivity.</abstract><pub>National Academy of Sciences</pub></addata></record> |
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title | Large-moment antiferromagnetic order in overdoped high-T c superconductor 154SmFeAsO1−xDₓ |
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