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Abstract
The kagome lattice is an intriguing and rich platform for discovering, tuning and understanding the diverse phases of quantum matter, crucial for advancing modern and future electronics. Despite considerable efforts, accessing correlated phases at room temperature has been challenging. Using single-crystal X-ray diffraction, we discovered charge order above room temperature in La(Ru1−xFex)3Si2 (x = 0, 0.01, 0.05), where charge order related to out-of-plane Ru atom displacements appears below TCO,I ≃ 400 K. The secondary charge ordered phase emerges below TCO,II ≃ 80–170 K. Furthermore, first principles calculations reveal both the kagome flat band and the van Hove point near the Fermi energy in LaRu3Si2, driven by Ru-dz2 orbitals. Our results identify LaRu3Si2 as the kagome superconductor with the highest known charge ordering temperature, offering a promising avenue for researching room temperature quantum phases and developing related technologies.
The study focuses on the charge order in LaRu3Si2, a material with a kagome lattice structure, discovering a charge-ordered state that persists at or above room temperature. This finding classifies LaRu3Si2 as the kagome superconductor with the highest charge ordering temperature, suggesting potential for applications in devices operating at normal environmental conditions without the need for cooling.
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1 Paul Scherrer Institut, Laboratory for Multiscale Materials Experiments, Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
2 Paul Scherrer Institute, Laboratory for Muon Spin Spectroscopy, Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501); Universität Zürich, Physik-Institut, Zürich, Switzerland (GRID:grid.7400.3) (ISNI:0000 0004 1937 0650)
3 University of Tokyo, Institute for Solid State Physics (ISSP), Kashiwa, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2169 1048)
4 Institute of Physics CAS, Praha, Czech Republic (GRID:grid.424881.3) (ISNI:0000 0004 0634 148X)
5 Huazhong University of Science and Technology, Wuhan National High Magnetic Field Center and School of Physics, Wuhan, China (GRID:grid.33199.31) (ISNI:0000 0004 0368 7223)
6 Paul Scherrer Institute, Laboratory for Muon Spin Spectroscopy, Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
7 Universität Zürich, Physik-Institut, Zürich, Switzerland (GRID:grid.7400.3) (ISNI:0000 0004 1937 0650)
8 Universität Zürich, Physik-Institut, Zürich, Switzerland (GRID:grid.7400.3) (ISNI:0000 0004 1937 0650); Faculty of Physics and Applied Computer Science, AGH University of Krakow, Kraków, Poland (GRID:grid.9922.0) (ISNI:0000 0000 9174 1488)
9 Deutsches Elektronen-Synchrotron DESY, Hamburg, Germany (GRID:grid.7683.a) (ISNI:0000 0004 0492 0453)
10 Princeton University, Laboratory for Topological Quantum Matter and Advanced Spectroscopy (B7), Department of Physics, Princeton, USA (GRID:grid.16750.35) (ISNI:0000 0001 2097 5006)
11 Southern University of Science and Technology, Department of Physics, Shenzhen, China (GRID:grid.263817.9) (ISNI:0000 0004 1773 1790)
12 University of Tokyo, Institute for Solid State Physics (ISSP), Kashiwa, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2169 1048); University of Tokyo, Department of Physics, Bunkyo-ku, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2169 1048)