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Abstract
Van Hove singularity (VHS) has been considered as a driving source for unconventional superconductivity. A VHS in two-dimensional (2D) materials consists of a saddle point connecting electron-like and hole-like bands. In a rare case, when a VHS appears at Fermi level, both electron-like and hole-like conduction can coexist, giving rise to an enhanced density of states as well as an attractive component of Coulomb interaction for unconventional electronic pairing. However, this van Hove scenario is often destroyed by an incorrect chemical potential or competing instabilities. Here, by using angle-resolved photoemission measurements, we report the observation of a VHS perfectly aligned with the Fermi level in a kagome superconductor CsV3-xTaxSb5 (x ~ 0.4), in which a record-high superconducting transition temperature is achieved among all the current variants of AV3Sb5 (A = Cs, Rb, K) at ambient pressure. Doping dependent measurements reveal the important role of van Hove scenario in boosting superconductivity, and spectroscopic-imaging scanning tunneling microscopy measurements indicate a distinct superconducting state in this system.
The authors present ARPES and STM/STS measurements of the kagome superconductor CsV3-xTaxSb5. For the x = 0.4 Ta-doped sample, they report evidence for a van Hove singularity perfectly aligned with the Fermi level, and that the superconducting transition temperature is maximized at this doping.
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1 University of Science and Technology of China, Department of Physics and CAS Key Laboratory of Strongly-coupled Quantum Matter Physics, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639)
2 Fuzhou University, Department of Physics, Fuzhou, China (GRID:grid.411604.6) (ISNI:0000 0001 0130 6528)
3 Beijing Institute of Technology, Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing, China (GRID:grid.43555.32) (ISNI:0000 0000 8841 6246); Beijing Institute of Technology, Beijing Key Lab of Nanophotonics and Ultrafine Optoelectronic Systems, Beijing, China (GRID:grid.43555.32) (ISNI:0000 0000 8841 6246)
4 Chinese Academy of Sciences, Beijing National Center for Condensed Matter Physics and Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000000119573309)
5 SLAC National Accelerator Laboratory, Stanford Synchrotron Radiation Lightsource, Menlo Park, USA (GRID:grid.445003.6) (ISNI:0000 0001 0725 7771)
6 University of Science and Technology of China, Department of Physics and CAS Key Laboratory of Strongly-coupled Quantum Matter Physics, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639); University of Science and Technology of China, International Center for Quantum Design of Functional Materials, Hefei, China (GRID:grid.59053.3a) (ISNI:0000000121679639)
7 Beijing Institute of Technology, Centre for Quantum Physics, Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement (MOE), School of Physics, Beijing, China (GRID:grid.43555.32) (ISNI:0000 0000 8841 6246); Beijing Institute of Technology, Beijing Key Lab of Nanophotonics and Ultrafine Optoelectronic Systems, Beijing, China (GRID:grid.43555.32) (ISNI:0000 0000 8841 6246); Yangtze Delta Region Academy of Beijing Institute of Technology, Material Science Center, Jiaxing, China (GRID:grid.43555.32) (ISNI:0000 0000 8841 6246)