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Abstract
Studies of single-spin objects are essential for designing emergent quantum states. We investigate a molecular magnet Tb2Pc3 interacting with a superconducting Pb(111) substrate, which hosts unprecedented Yu-Shiba-Rusinov (YSR) subgap states, dubbed spin-orbital YSR states. Upon adsorption of the molecule on Pb, the degeneracy of its lowest unoccupied molecular orbitals (LUMO) is lifted, and the lower LUMO forms a radical spin via charge transfer. This leads to Kondo screening and subgap states. Intriguingly, the YSR states display two pairs of resonances with clearly distinct behavior. The energy of the inner pair exhibits prominent inter and intra molecular variation, and it strongly depends on the tip height. The outer pair, however, shifts only slightly. As is unveiled through theoretical calculations, the two pairs of YSR states originate from the ligand spin and charge-fluctuating higher LUMO, coexisting in a single molecule, but only weakly coupled presumably due to different spatial distribution. Our work paves the way for understanding complex many-body excitations and constructing molecule-based topological superconductivity.
Yu-Shiba-Rusinov (YSR) states result from the exchange coupling between a localized magnetic moment and a superconductor. Traditionally, the YSR states have been studied for magnetic atoms. For molecular magnets with extended ligand spin, the entanglement of spin and ligand orbital gives rise to new forms of YSR excitations. Here, Xia et al uncovered spin-orbital YSR states in an unpaired ligand spin in the molecular magnet Tb2Pc3 on Pb.
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1 Huazhong University of Science and Technology, School of Physics and Wuhan National High Magnetic Field Center, Wuhan, China (GRID:grid.33199.31) (ISNI:0000 0004 0368 7223)
2 Institute for Molecular Science, Okazaki, Japan (GRID:grid.467196.b) (ISNI:0000 0001 2285 6123); Osaka University, The Institute for Scientific and Industrial Research, Ibaraki, Japan (GRID:grid.136593.b) (ISNI:0000 0004 0373 3971)
3 Jožef Stefan Institute, Ljubljana, Slovenia (GRID:grid.11375.31) (ISNI:0000 0001 0706 0012); University of Ljubljana, Faculty of Mathematics and Physics, Ljubljana, Slovenia (GRID:grid.8954.0) (ISNI:0000 0001 0721 6013)
4 Institute of Nanotechnology (INT), Karlsruhe Institute of Technology (KIT), Eggenstein-Leopoldshafen, Germany (GRID:grid.7892.4) (ISNI:0000 0001 0075 5874)
5 Institute of Nanotechnology (INT), Karlsruhe Institute of Technology (KIT), Eggenstein-Leopoldshafen, Germany (GRID:grid.7892.4) (ISNI:0000 0001 0075 5874); Karlsruhe Institute of Technology (KIT), Institute for Quantum Materials and Technologies (IQMT), Eggenstein-Leopoldshafen, Germany (GRID:grid.7892.4) (ISNI:0000 0001 0075 5874); Institut de Science et d’Ingénierie Supramoléculaires (ISIS), Centre Européen de Sciences Quantiques (CESQ), Strasbourg Cedex, France (GRID:grid.483413.9) (ISNI:0000 0004 0452 5875)
6 Huazhong University of Science and Technology, School of Physics and Wuhan National High Magnetic Field Center, Wuhan, China (GRID:grid.33199.31) (ISNI:0000 0004 0368 7223); Huazhong University of Science and Technology, Hubei Key Laboratory of Gravitation and Quantum Physics, Wuhan, China (GRID:grid.33199.31) (ISNI:0000 0004 0368 7223)