TY - JOUR
T1 - Maximizing T c by tuning nematicity and magnetism in FeSe1-x S x superconductors
AU - Matsuura, K.
AU - Mizukami, Y.
AU - Arai, Y.
AU - Sugimura, Y.
AU - Maejima, N.
AU - Machida, A.
AU - Watanuki, T.
AU - Fukuda, T.
AU - Yajima, T.
AU - Hiroi, Z.
AU - Yip, K. Y.
AU - Chan, Y. C.
AU - Niu, Q.
AU - Hosoi, S.
AU - Ishida, K.
AU - Mukasa, K.
AU - Kasahara, S.
AU - Cheng, J. G.
AU - Goh, S. K.
AU - Matsuda, Y.
AU - Uwatoko, Y.
AU - Shibauchi, T.
N1 - Funding Information:
We thank H. Kontani and Y. Yamakawa for fruitful discussions. We also thank S. Nagasaki and T. Watashige for technical assistance. This work was performed using facilities of the Institute for Solid State Physics, the University of Tokyo. A part of this work was performed under the Shared Use Program of JAEA and QST Facilities (Proposal No. 2015A-E16, 2016A-E16, and 2016B-H13) supported by JAEA, QST Advanced Characterization Nanotechnology Platform as a program of “Nanotechnology Platform” of the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan (Proposal No. A-15-AE-0016, A-16-QS-0008, and A-16-QS-0025). The synchrotron radiation experiments were performed by using a QST experimental station at JAEA beamline BL22XU in SPring-8 with the approval of the Japan Synchrotron Radiation Research Institute (JASRI) (Proposal No. 2015A3701, 2015A3783, 2015B3701, 2016A3751, 2016A3781 and 2016B3785). This work was supported by Grant-in-Aids for Scientific Research (A), (B), (S), (Proposal No. 15H02106, 15H03681, 15H03688, and 25220710) and Grant-in-Aid for Young Scientists (B) (Proposal No. 15K17692) from Japan Society for the Promotion of Science (JSPS), Grant-in-Aids on Innovative Areas “Topological Materials Science” (No. 15H05852) from MEXT, CUHK Startup Grant (No. 4930048), and Research Grant Council of Hong Kong (ECS/24300214, GRF/ 14301316). J.-G.C. acknowledges the supported from the NSFC, MOST, and CAS (Proposal No. 11574377, 2014CB921500, XDB07020100 and QYZDB-SSW-SLH013).
Publisher Copyright:
© 2017 The Author(s).
PY - 2017/12/1
Y1 - 2017/12/1
N2 - A fundamental issue concerning iron-based superconductivity is the roles of electronic nematicity and magnetism in realising high transition temperature (T c). To address this issue, FeSe is a key material, as it exhibits a unique pressure phase diagram involving non-magnetic nematic and pressure-induced antiferromagnetic ordered phases. However, as these two phases in FeSe have considerable overlap, how each order affects superconductivity remains perplexing. Here we construct the three-dimensional electronic phase diagram, temperature (T) against pressure (P) and isovalent S-substitution (x), for FeSe1-x S x . By simultaneously tuning chemical and physical pressures, against which the chalcogen height shows a contrasting variation, we achieve a complete separation of nematic and antiferromagnetic phases. In between, an extended non-magnetic tetragonal phase emerges, where T c shows a striking enhancement. The completed phase diagram uncovers that high-T c superconductivity lies near both ends of the dome-shaped antiferromagnetic phase, whereas T c remains low near the nematic critical point.
AB - A fundamental issue concerning iron-based superconductivity is the roles of electronic nematicity and magnetism in realising high transition temperature (T c). To address this issue, FeSe is a key material, as it exhibits a unique pressure phase diagram involving non-magnetic nematic and pressure-induced antiferromagnetic ordered phases. However, as these two phases in FeSe have considerable overlap, how each order affects superconductivity remains perplexing. Here we construct the three-dimensional electronic phase diagram, temperature (T) against pressure (P) and isovalent S-substitution (x), for FeSe1-x S x . By simultaneously tuning chemical and physical pressures, against which the chalcogen height shows a contrasting variation, we achieve a complete separation of nematic and antiferromagnetic phases. In between, an extended non-magnetic tetragonal phase emerges, where T c shows a striking enhancement. The completed phase diagram uncovers that high-T c superconductivity lies near both ends of the dome-shaped antiferromagnetic phase, whereas T c remains low near the nematic critical point.
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U2 - 10.1038/s41467-017-01277-x
DO - 10.1038/s41467-017-01277-x
M3 - Article
C2 - 29070845
AN - SCOPUS:85032296227
SN - 2041-1723
VL - 8
JO - Nature communications
JF - Nature communications
IS - 1
M1 - 1143
ER -