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Pure nematic state in the iron-based superconductor FeSe

Y. Kubota1,*, F. Nabeshima2, K. Nakayama3,4, H. Ohsumi1, Yoshikazu Tanaka1, K. Tamasaku1,5, T. Suzuki6, K. Okazaki6, T. Sato3,7 et al.

A. Maeda2 and M. Yabashi1,5

  • 1RIKEN SPring-8 Center, 1-1-1 Kouto, Sayo, Hyogo 679-5148, Japan
  • 2Department of Basic Science, University of Tokyo, 3-8-1 Komaba, Meguro, Tokyo 153-8902, Japan
  • 3Department of Physics, Graduate School of Science, Tohoku University, Sendai 980-8578, Japan
  • 4Precursory Research for Embryonic Science and Technology, Japan Science and Technology Agency, Tokyo 102-0076, Japan
  • 5Japan Synchrotron Radiation Research Institute (JASRI), 1-1-1 Kouto, Sayo, Hyogo 679-5198, Japan
  • 6Institute for Solid State Physics, The University of Tokyo, Kashiwa, Chiba 277-8581, Japan
  • 7Advanced Institute for Materials Research (WPI-AIMR), Tohoku University, Sendai 980-8577, Japan

  • *kubota@spring8.or.jp

Phys. Rev. B 108, L100501 – Published 5 September, 2023

DOI: https://doi.org/10.1103/PhysRevB.108.L100501

Abstract

Lattice and electronic states of thin FeSe films on LaAlO3 substrates are investigated in the vicinity of the nematic phase transition. No evidence of a structural phase transition is found by x-ray diffraction below T*∼90 K, while results obtained from a resistivity measurement and angle-resolved photoemission spectroscopy clearly show the appearance of a nematic state. These results indicate the formation of a pure nematic state in the iron-based superconductor and provide conclusive evidence that the nematic state originates from the electronic degrees of freedom. This pure nematicity in the thin film implies the difference in the electron-lattice interaction from bulk FeSe crystals. FeSe films provide valuable playgrounds for observing the pure response of “bare” electron systems free from the electron-lattice interaction, and should make an important contribution to investigate nematicity and its relationship with superconductivity.

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