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We use density functional theory to calculate the electronic band structures, cohesive energies, phonon dispersions, and optical absorption spectra of two-dimensional In₂X₂ crystals, where X is S, Se, or Te. We identify two crystalline phases (and) of monolayers of hexagonal In₂X₂, and show that they are characterized by different sets of Raman-active phonon modes. We find that these materials are indirect-band-gap semiconductors with a sombrero-shaped dispersion of holes near the valence-band edge. The latter feature results in a Lifshitz transition (a change in the Fermi-surface topology of hole-doped In₂X₂) at hole concentrations nₒ=6. 8610^13 cm^-2, nₒ₄=6. 2010^13 cm^-2, and nₓ₄=2. 8610^13 cm^-2 for X=S, Se, and Te, respectively, for -In₂X₂ and nₒ=8. 3210^13 cm^-2, nₒ₄=6. 0010^13 cm^-2, and nₓ₄=8. 1410^13 cm^-2 for -In₂X₂.
Zólyomi et al. (Wed,) studied this question.