Figure 3.
(a) Dyson orbitals of a typical valence state, s SAMO, p SAMO and d SAMO states of Ho3N@C80 with an isocontour of 0.002|e|/Å. (b) Charge density of the Dyson orbitals of panel a. (c) Density of SAMO states as a function of the excitation energy. The electronic states and Dyson orbitals have been computed in TDDFT at the LC-BLYP/6–31G(d) + ECP56MWB/7s6p5d for Ho + Bq (6–31(6+)G(d)) level for Ho3N@C80’s lowest energy isomer shown in the inset.