Author
Listed:
- Md Shafayat Hossain
(Princeton University)
- Qi Zhang
(Princeton University)
- David Graf
(National High Magnetic Field Laboratory)
- Mikel Iraola
(Donostia International Physics Center
Institute for Theoretical Solid State Physics, IFW Dresden)
- Tobias Müller
(University of Zurich)
- Sougata Mardanya
(Howard University)
- Yi-Hsin Tu
(National Cheng Kung University)
- Zhuangchai Lai
(City University of Hong Kong
The Hong Kong Polytechnic University)
- Martina O. Soldini
(University of Zurich)
- Siyuan Li
(City University of Hong Kong)
- Yao Yao
(City University of Hong Kong)
- Yu-Xiao Jiang
(Princeton University)
- Zi-Jia Cheng
(Princeton University)
- Maksim Litskevich
(Princeton University)
- Brian Casas
(National High Magnetic Field Laboratory)
- Tyler A. Cochran
(Princeton University)
- Xian P. Yang
(Princeton University)
- Byunghoon Kim
(Princeton University)
- Kenji Watanabe
(National Institute for Materials Science)
- Takashi Taniguchi
(National Institute for Materials Science)
- Sugata Chowdhury
(Howard University)
- Arun Bansil
(Northeastern University
Northeastern University)
- Hua Zhang
(City University of Hong Kong
City University of Hong Kong
City University of Hong Kong
City University of Hong Kong)
- Tay-Rong Chang
(National Cheng Kung University
Center for Quantum Frontiers of Research and Technology (QFort)
National Center for Theoretical Sciences)
- Mark H. Fischer
(University of Zurich)
- Titus Neupert
(University of Zurich)
- Luis Balicas
(National High Magnetic Field Laboratory
Florida State University)
- M. Zahid Hasan
(Princeton University
Quantum Science Center at ORNL)
Abstract
Transition metal dichalcogenides display a high technological potential due to their wide range of electronic ground states. Here, we unveil that by tuning hydrostatic pressure P, a cascade of electronic phase transitions can be induced in the few-layer transition metal dichalcogenide 1T’-WS2. As P increases, we observe the suppression of superconductivity with the concomitant emergence of an anomalous Hall effect (AHE) at $$P\approx 1.15$$ P ≈ 1.15 GPa. Above 1.6GPa, we uncover a reentrant superconducting state emerging from a state still exhibiting AHE. This superconducting state competes with the AHE state and shows a marked increase in superconducting anisotropy with respect to the ambient pressure phase, suggesting a distinct pairing symmetry. We demonstrate that 1T’-WS2 concomitantly transitions into a strong topological phase with different band orbital characters and Fermi surfaces contributing to the superconductivity. These findings position 1T’-WS2 as a tunable superconductor, wherein superconductivity, AHE, and band features can be tuned reversibly.
Suggested Citation
Md Shafayat Hossain & Qi Zhang & David Graf & Mikel Iraola & Tobias Müller & Sougata Mardanya & Yi-Hsin Tu & Zhuangchai Lai & Martina O. Soldini & Siyuan Li & Yao Yao & Yu-Xiao Jiang & Zi-Jia Cheng & , 2025.
"Tunable superconductivity coexisting with the anomalous Hall effect in a transition metal dichalcogenide,"
Nature Communications, Nature, vol. 16(1), pages 1-9, December.
Handle:
RePEc:nat:natcom:v:16:y:2025:i:1:d:10.1038_s41467-025-56919-2
DOI: 10.1038/s41467-025-56919-2
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