Wigner-molecule supercrystal in transition-metal dichalcogenide moiré superlattices: Lessons from the bottom-up approach
arXiv:2403.12262 · doi:10.1103/PhysRevB.109.L121302
Abstract
The few-body problem for fermionic charge carriers in a double-well moiré quantum dot (MQD), representing the first step in a bottom-up strategy to investigate formation of molecular supercrystals in transition metal dichalcogenide (TMD) moiré superlattices with integral fillings, , is solved exactly by employing large-scale exact-diagonalization via full configuration interaction (FCI) computations. A comparative analysis with the mean-field solutions of the often used spin-and-space unrestricted Hartree Fock (sS-UHF) demonstrates the limitations of the UHF method (by itself) to provide a proper description of the influence of the interdot Coulomb interaction. In particular, it is explicitly shown for that the exact charge densities (CDs) within each MQD retain the ring-like shape characteristic (for a wide range of relevant parameters) of a fully isolated MQD, as was found for sliding Wigner molecules (WMs). This deeply quantum-mechanical behavior contrasts sharply with the UHF CDs that portray solely orientationally pinned and well localized dumbbell dimers. An improved CD, which agrees with the FCI-calculated one, derived from the restoration of the sS-UHF broken parity symmetries is further introduced, suggesting a beyond-mean-field methodological roadmap for correcting the sS-UHF results. It is conjectured that the conclusions for the moiré TMD superlattice case extend to all cases with integral fillings that are associated with sliding WMs in isolated MQDs. The case of , associated with a pinned WM in isolated MQDs, is an exception.
arXiv comment9-page Letter with 5 color figures. For related papers, see https://sites.gatech.edu/cyannouleas/
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