Nematic, chiral, and topological superconductivity in twisted transition metal dichalcogenides
Constantin Schrade, Liang Fu
DOI 10.1103/PhysRevB.110.035143 · Physical Review B
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Abstract
We introduce and study a realistic model for superconductivity in twisted bilayer WSe2, where electron pairing arises from spin-valley fluctuations in the weak-coupling regime. Our model comprises both the full continuum model moiré band structure and a short-ranged repulsive interaction. By calculating the spin-valley susceptibility, we identify a significant enhancement of the spin-valley fluctuations near half filling of the topmost moiré band. We then analyze the dominant Kohn-Luttinger pairing instabilities due to these spin-valley fluctuations and show that the leading instability corresponds to a two-component order parameter, which can give rise to nematic, chiral, and topological superconductivity. As our findings are asymptotically exact for small interaction strengths, they provide a viable starting point for future studies of superconductivity in twisted transition metal dichalcogenide bilayers.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| WSe2 Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
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