Twist-angle evolution of the intervalley-coherent antiferromagnet in twisted WSe
arXiv:2503.11763 · doi:10.1103/m6c2-yd5j
Abstract
Recent experimental reports of correlated physics in twisted homobilayer WSe have spurred interest in the interplay of electronic interactions and topology in this system. Here, we explore its phase diagram using the Hartree-Fock approximation within a three-orbital Wannier model of the bilayer. Our analysis reveals a dominant intervalley-coherent antiferromagnetic instability, whose stability in the space of twist angle, interaction strength, out-of-plane displacement field, and hole density is primarily set by nesting and commensurability. At large angles or low interaction-to-bandwidth ratios, the instability arises at hole densities above half filling near a van-Hove line where the strong Fermi surface nesting occurs due to the flatness of the band in a region enclosing the van-Hove and points. Increasing interaction strength or decreasing the twist angle gradually shifts the ordered phase toward half filling, where the strongest antiferromagnetic order gets pinned due to commensurability effects that enable a full gap opening. The antiferromagnetic order parameter strongly couples to the layer polarization, which makes its transition to the normal state sharp in the strong-coupling limit and carries implications for collective modes. Our Hartree-Fock phase diagram reproduces key aspects of recent experiments and the reconstructed Fermi surfaces and DOS in the antiferromagnetic phase account for subtle transport signatures observed in these studies.
11+15 pages, 7+14 figures
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