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  • Letter
  • Open Access

Optimal superconductivity in twisted bilayer WSe2 where the Van Hove singularity crosses half-filling

Michał Zegrodnik1,*, Waseem Akbar1, Andrzej Biborski1, and Louk Rademaker2,3

  • 1Academic Centre for Materials and Nanotechnology, AGH University of Krakow, Al. Mickiewicza 30, 30-059 Krakow, Poland
  • 2Department of Theoretical Physics, University of Geneva, CH-1211 Geneva, Switzerland
  • 3Institute-Lorentz for Theoretical Physics, Leiden University, P.O. Box 9506, Leiden NL-2300, The Netherlands

  • *Contact author: michal.zegrodnik@agh.edu.pl

Phys. Rev. Research 8, L012070 – Published 25 March, 2026

DOI: https://doi.org/10.1103/pkf3-fkv4

Abstract

The recent discovery of unconventional superconductivity has pointed to twisted WSe2 bilayer as a versatile platform for studying the correlated and topological phases of matter. Here, we analyze the effect of the displacement field and electron interactions on the formation of a topological paired state in twisted WSe2. Our approach is based on the effective single band t−J−U model supplemented with intersite Coulomb interaction term and treated within the Gutzwiller approximation. We show that the superconducting phase is stabilized in a small range of displacement fields where the Van Hove singularity crosses half-filling, which is in qualitative agreement with recent experimental data. According to our analysis, such a circumstance comes as a result of a subtle interplay between the large density of states of the Van Hove singularity, in combination with the renormalization effects that appear in the weak-to-moderate correlation regime. The two factors create favorable conditions for the superconducting pairing only in a small area of the phase diagram.

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