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Abstract
Finding d-electron heavy fermion states has been an important topic as the diversity in d-electron materials can lead to many exotic Kondo effect-related phenomena or new states of matter such as correlation-driven topological Kondo insulator. Yet, obtaining direct spectroscopic evidence for a d-electron heavy fermion system has been elusive to date. Here, we report the observation of Kondo lattice behavior in an antiferromagnetic metal, FeTe, via angle-resolved photoemission spectroscopy, scanning tunneling spectroscopy and transport property measurements. The Kondo lattice behavior is represented by the emergence of a sharp quasiparticle and Fano-type tunneling spectra at low temperatures. The transport property measurements confirm the low-temperature Fermi liquid behavior and reveal successive coherent-incoherent crossover upon increasing temperature. We interpret the Kondo lattice behavior as a result of hybridization between localized Fe 3dxy and itinerant Te 5pz orbitals. Our observations strongly suggest unusual cooperation between Kondo lattice behavior and long-range magnetic order.
The Kondo hybridization typically occurs in heavy-fermion systems containing f electrons, although recently it has been reported in d-electron systems. Kim et al. report spectroscopic evidence of the Kondo hybridization in FeTe and discuss it role in the mechanism of the magnetic order.
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1 Institute for Basic Science, Center for Correlated Electron Systems, Seoul, Korea (GRID:grid.410720.0) (ISNI:0000 0004 1784 4496); Seoul National University, Department of Physics & Astronomy, Seoul, Korea (GRID:grid.31501.36) (ISNI:0000 0004 0470 5905)
2 DGIST, Department of Emerging Materials Science, Daegu, Korea (GRID:grid.417736.0) (ISNI:0000 0004 0438 6721)
3 Pohang University of Science and Technology (POSTECH), Department of Chemistry, Pohang, Korea (GRID:grid.49100.3c) (ISNI:0000 0001 0742 4007)
4 Korea Institute for Advanced Study, Seoul, Korea (GRID:grid.249961.1) (ISNI:0000 0004 0610 5612)
5 National Synchrotron Radiation Research Center, Hsinchu, Taiwan (GRID:grid.410766.2) (ISNI:0000 0001 0749 1496)
6 Kyungpook National University, Department of Physics, Daegu, Korea (GRID:grid.258803.4) (ISNI:0000 0001 0661 1556)
7 SLAC National Accelerator Laboratory, Stanford Synchrotron Radiation Light Source, Menlo Park, USA (GRID:grid.445003.6) (ISNI:0000 0001 0725 7771)
8 Yonsei University, Department of Physics, Seoul, Korea (GRID:grid.15444.30) (ISNI:0000 0004 0470 5454)
9 Chinese Academy of Sciences, Center for Excellence in Superconducting Electronics, State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology, Shanghai, China (GRID:grid.9227.e) (ISNI:0000000119573309)
10 Institute for Basic Science, Center for Correlated Electron Systems, Seoul, Korea (GRID:grid.410720.0) (ISNI:0000 0004 1784 4496); Seoul National University, Department of Physics & Astronomy, Seoul, Korea (GRID:grid.31501.36) (ISNI:0000 0004 0470 5905); Massachusetts Institute of Technology, Department of Physics, Cambridge, USA (GRID:grid.116068.8) (ISNI:0000 0001 2341 2786)
11 Chinese Academy of Sciences, Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000 0001 1957 3309); University of Chinese Academy of Sciences, School of Physical Sciences, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419); Songshan Lake Materials Laboratory, Dongguan, China (GRID:grid.511002.7)
12 Pohang Accelerator Laboratory, XFEL Beamline Division, Pohang, Korea (GRID:grid.15444.30) (ISNI:0000 0004 0632 5770)
13 Sungkyunkwan University, Department of Physics, Suwon, Korea (GRID:grid.264381.a) (ISNI:0000 0001 2181 989X)