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Abstract
Determining the pairing symmetry of single-layer FeSe on SrTiO3 is the key to understanding the enhanced pairing mechanism. It also guides the search for superconductors with high transition temperatures. Despite considerable efforts, it remains controversial whether the symmetry is the sign-preserving s- or the sign-changing s±-wave. Here, we investigate the pairing symmetry of single-layer FeSe from a topological point of view. Using low-temperature scanning tunneling microscopy/spectroscopy, we systematically characterize the superconducting states at edges and corners of single-layer FeSe. The tunneling spectra collected at edges and corners show a full energy gap and a substantial dip, respectively, suggesting the absence of topologically non-trivial edge and corner modes. According to our theoretical calculations, these spectroscopic features can be considered as strong evidence for the sign-preserving s-wave pairing in single-layer FeSe.
The nature of the pairing symmetry in superconducting single-layer FeSe has been the subject of intense debate. Here, the authors use scanning tunneling microscopy/spectroscopy to show the absence of topological edge/corner modes, providing evidence for sign-preserving s-wave pairing.
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1 Southern University of Science and Technology, Department of Physics, Shenzhen, China (GRID:grid.263817.9) (ISNI:0000 0004 1773 1790); Tsinghua University, State Key Laboratory of Low-Dimensional Quantum Physics, Department of Physics, Beijing, China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178)
2 Beijing Institute of Technology, School of Physics, Beijing, China (GRID:grid.43555.32) (ISNI:0000 0000 8841 6246); University of Chinese Academy of Sciences, Kavli Institute of Theoretical Sciences, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419); University of Chinese Academy of Sciences, CAS Center for Excellence in Topological Quantum Computation, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419)
3 Tsinghua University, State Key Laboratory of Low-Dimensional Quantum Physics, Department of Physics, Beijing, China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178); Beijing Academy of Quantum Information Sciences, Beijing, China (GRID:grid.510904.9) (ISNI:0000 0004 9362 2406)
4 Chinese Academy of Sciences, CAS Key Laboratory of Theoretical Physics, Institute of Theoretical Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000000119573309)
5 University of Chinese Academy of Sciences, Kavli Institute of Theoretical Sciences, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419); University of Chinese Academy of Sciences, CAS Center for Excellence in Topological Quantum Computation, Beijing, China (GRID:grid.410726.6) (ISNI:0000 0004 1797 8419); Chinese Academy of Sciences, Beijing National Research Center for Condensed Matter Physics, and Institute of Physics, Beijing, China (GRID:grid.9227.e) (ISNI:0000 0001 1957 3309)
6 Southern University of Science and Technology, Department of Physics, Shenzhen, China (GRID:grid.263817.9) (ISNI:0000 0004 1773 1790); Quantum Science Center of Guangdong–Hong Kong–Macao Greater Bay Area (Guangdong), Shenzhen, China (GRID:grid.263817.9)
7 Tsinghua University, State Key Laboratory of Low-Dimensional Quantum Physics, Department of Physics, Beijing, China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178)
8 Southern University of Science and Technology, Department of Physics, Shenzhen, China (GRID:grid.263817.9) (ISNI:0000 0004 1773 1790); Tsinghua University, State Key Laboratory of Low-Dimensional Quantum Physics, Department of Physics, Beijing, China (GRID:grid.12527.33) (ISNI:0000 0001 0662 3178); Beijing Academy of Quantum Information Sciences, Beijing, China (GRID:grid.510904.9) (ISNI:0000 0004 9362 2406); Quantum Science Center of Guangdong–Hong Kong–Macao Greater Bay Area (Guangdong), Shenzhen, China (GRID:grid.510904.9)