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Edwards B, Dowinton O, Hall AE, Murgatroyd PAE, Buchberger S, Antonelli T, Siemann GR, Rajan A, Morales EA, Zivanovic A, Bigi C, Belosludov RV, Polley CM, Carbone D, Mayoh DA, Balakrishnan G, Bahramy MS, King PDC. Giant valley-Zeeman coupling in the surface layer of an intercalated transition metal dichalcogenide. Nat Mater 2023; 22:459-465. [PMID: 36658327 DOI: 10.1038/s41563-022-01459-z] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/04/2022] [Accepted: 12/06/2022] [Indexed: 06/17/2023]
Abstract
Spin-valley locking is ubiquitous among transition metal dichalcogenides with local or global inversion asymmetry, in turn stabilizing properties such as Ising superconductivity, and opening routes towards 'valleytronics'. The underlying valley-spin splitting is set by spin-orbit coupling but can be tuned via the application of external magnetic fields or through proximity coupling. However, only modest changes have been realized to date. Here, we investigate the electronic structure of the V-intercalated transition metal dichalcogenide V1/3NbS2 using microscopic-area spatially resolved and angle-resolved photoemission spectroscopy. Our measurements and corresponding density functional theory calculations reveal that the bulk magnetic order induces a giant valley-selective Ising coupling exceeding 50 meV in the surface NbS2 layer, equivalent to application of a ~250 T magnetic field. This energy scale is of comparable magnitude to the intrinsic spin-orbit splittings, and indicates how coupling of local magnetic moments to itinerant states of a transition metal dichalcogenide monolayer provides a powerful route to controlling their valley-spin splittings.
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Affiliation(s)
- B Edwards
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK
| | - O Dowinton
- Department of Physics and Astronomy, University of Manchester, Manchester, UK
| | - A E Hall
- Department of Physics, University of Warwick, Coventry, United Kingdom
| | - P A E Murgatroyd
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK
| | - S Buchberger
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK
- Max Planck Institute for Chemical Physics of Solids, Dresden, Germany
| | - T Antonelli
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK
| | - G-R Siemann
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK
| | - A Rajan
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK
| | - E Abarca Morales
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK
- Max Planck Institute for Chemical Physics of Solids, Dresden, Germany
| | - A Zivanovic
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK
- Max Planck Institute for Chemical Physics of Solids, Dresden, Germany
| | - C Bigi
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK
| | - R V Belosludov
- Institute for Materials Research, Tohoku University, Sendai, Japan
| | - C M Polley
- MAX IV Laboratory, Lund University, Lund, Sweden
| | - D Carbone
- MAX IV Laboratory, Lund University, Lund, Sweden
| | - D A Mayoh
- Department of Physics, University of Warwick, Coventry, United Kingdom
| | - G Balakrishnan
- Department of Physics, University of Warwick, Coventry, United Kingdom
| | - M S Bahramy
- Department of Physics and Astronomy, University of Manchester, Manchester, UK.
| | - P D C King
- SUPA, School of Physics and Astronomy, University of St Andrews, St Andrews, UK.
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