Nematic, chiral and topological superconductivity in transition metal dichalcogenides
arXiv:2110.10172 · doi:10.1103/PhysRevB.110.035143
Abstract
We introduce and study a realistic model for superconductivity in twisted bilayer WSe, where electron pairing arises from spin-valley fluctuations in the weak-coupling regime. Our model comprises both the full continuum model moiré bandstructure and a short-ranged repulsive interaction. By calculating the spin-valley susceptibility, we identify a Fermi surface nesting feature near half-filling of the top-most moiré band, which induces significantly enhanced spin-valley fluctuations. 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.
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- Superconductivity in twisted WSe from topology-induced quantum fluctuations
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