Answers are grounded in this paper and cite their sources.
Fulleride crystals ( M 3 C 60 ) are materials whose electrical transport properties are influenced by the distinct structural environments of their tetrahedral and octahedral interstitial doping sites. In this work, the chemical bond overlap model (OP/TOP), the quantum theory of atoms in molecules (QTAIM), and molecular descriptors were utilized to investigate M ⋯ C 60 interactions. Representative clusters modeling isolated tetrahedral M ( C 60 ) 4 and octahedral M ( C 60 ) 6 environments ( M = Li, Na, K, Rb, Cs ) were investigated using density functional theory at the ω B97X-D3/def2-SVP level. Molecular descriptors reveal that alkali-metal doping decrease the HOMO-LUMO gap ( Δ E HL ), and both the ionization potential ( I P ) and chemical hardness ( η ). For all metals except Rb, the octahedral models exhibited lower HOMO-LUMO gaps and I P than the corresponding tetrahedral models. QTAIM and OP/TOP descriptors indicate that the M-C bonds within the tetrahedral sites exhibit ionic behavior characterized by interatomic charge depletion ( ∇ 2 ρ BCP > 0 , H BCP > 0 ) and highly concentrated overlap density ( ∇ 2 ρ OCP ≪ 0 ). In contrast, the octahedral sites feature delocalized electron overlap profiles. The combined QTAIM and OP/TOP analyses indicate distinct electronic structure for the two interstitial environments: tetrahedral sites are associated with stronger charge-transfer characteristics, whereas octahedral sites display more spatially distributed electron density.
No takes yet. Share an insight, caveat, or question.
Fonseca et al. (2026) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: