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3 Pith papers cite this work. Polarity classification is still indexing.

3 Pith papers citing it

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2026 2 2025 1

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UNVERDICTED 3

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Self-doped Crystal from Preempted Band-inversion Transitions

cond-mat.str-el · 2026-04-10 · unverdicted · novelty 7.0

Self-doped Wigner crystals arise from preempted band-inversion transitions between commensurate crystals, as established by non-perturbative arguments and Hartree-Fock calculations in jellium and rhombohedral graphene models.

General Many-Body Perturbation Framework for Moir\'e Systems

cond-mat.str-el · 2025-09-24 · unverdicted · novelty 6.0

A GW+RPA perturbation framework built on Hartree-Fock is applied to hBN-aligned rhombohedral pentalayer graphene and magic-angle twisted bilayer graphene, producing phase diagrams and spectra that match experiments and predicting a nematic metal ground state at charge neutrality in MATBG.

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Showing 3 of 3 citing papers.

  • Self-doped Crystal from Preempted Band-inversion Transitions cond-mat.str-el · 2026-04-10 · unverdicted · none · ref 35

    Self-doped Wigner crystals arise from preempted band-inversion transitions between commensurate crystals, as established by non-perturbative arguments and Hartree-Fock calculations in jellium and rhombohedral graphene models.

  • Valley polarization of chiral excitonic bound states induced by band geometry cond-mat.mes-hall · 2026-04-06 · unverdicted · none · ref 49

    Berry flux in double-well dispersions can drive chiral excitonic condensates with evolving angular momentum channels, and trigonal warping in multilayer graphene leads to mixed angular momentum ground states.

  • General Many-Body Perturbation Framework for Moir\'e Systems cond-mat.str-el · 2025-09-24 · unverdicted · none · ref 47

    A GW+RPA perturbation framework built on Hartree-Fock is applied to hBN-aligned rhombohedral pentalayer graphene and magic-angle twisted bilayer graphene, producing phase diagrams and spectra that match experiments and predicting a nematic metal ground state at charge neutrality in MATBG.