Systematic analysis reveals strong screening and charge-density-wave instabilities in two-dimensional materials, indicating potential for unique electronic behaviors.
Understanding the interplay between screening, electronic correlations, and collective excitations is essential for the design of two-dimensional quantum materials. Here, we present a comprehensive first-principles study of more than 60 MA 2 Z 4 monolayers, encompassing semiconducting, metallic, cold-metallic, magnetic, and topological phases. Using the constrained random phase approximation (cRPA), we compute material-specific effective Coulomb interaction parameters U , U^ U ′ , and J , including their spatial dependence across distinct correlated subspaces defined by local coordination and crystal symmetry. In semiconducting compounds, long-range nonlocal interactions persist, revealing unconventional screening and suggesting strong excitonic effects beyond simple dielectric models. In cold-metallic systems, sizable long-range Coulomb interactions remain despite the presence of free carriers, highlighting their atypical metallic screening. Among 33-valence-electron compounds, we find Uᵉᶠᶠ\,>\,W U eff > W in the β 2 phase, indicating proximity to charge-density-wave or Mott instabilities. Several V- and Nb-based systems exhibit intermediate-to-strong correlation strength, with U / W > 1 in multiple cases. Using cRPA-derived Stoner parameters, we identify magnetic instabilities in various V-, Nb-, Cr-, and Mn-based compounds. Finally, selected cold-metallic systems display plasmon dispersions that deviate from the conventional √q q behavior, revealing nearly non-dispersive low-energy modes. These results position MA 2 Z 4 monolayers as a versatile platform for investigating correlation-driven instabilities and emergent collective behavior in two dimensions.
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Bagherpour et al. (2025) studied this question.
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