Abstract
Density functional theory (DFT) and time-dependent density functional theory (TD-DFT) calculations are carried out to study the stabilities, photoelectron, infrared, Raman and electronic absorption spectra of borospherene B44− and metalloborospherenes MB440/− (M = Li, Na, and K). It is found that all atoms can form stable exohedral metalloborospherenes M&B440/−, whereas only Na and K atoms can be stably encapsulated inside B440/− cage. In addition, relative energies of these metalloborospherenes suggest that Na and K atoms favor exohedral configuration. Importantly, doping of metal atom can modify the stabilities of B44 with different structures, which provides a possible route to produce stable boron clusters or metalloborospherenes. The calculated results suggest that B44 tends to get electrons from the doped metal. Metalloborospherenes MB44− are characterized as charge-transfer complexes (M2+B442−), where B44 tends to get two electrons from the extra electron and the doped metal, resulting in similar features with anionic B442−. In addition, doping of metal atom can change the spectral features, such as blueshift or redshift and weakening or strengthening of characteristic peaks, since the extra metal atom can modify the electronic structure. The calculated spectra are readily compared with future spectroscopy measurements and can be used as fingerprints to identify B44− and metalloborospherenes.
Highlights
Density functional theory (DFT) and time-dependent density functional theory (TD-DFT) calculations are carried out to study the stabilities, photoelectron, infrared, Raman and electronic absorption spectra of borospherene B44− and metalloborospherenes MB440/− (M = Li, Na, and K)
Photoelectron spectroscopy analysis indicated that combination of the simulated photoelectron spectra of cage B40− and quasi-planar B40− can reproduce the observed spectrum, which confirmed the existence of cage B40−
The structure search algorithms and DFT combined approaches have been used and the low-lying structures of boron clusters have been reported by many authors[26,28,29,30,44]
Summary
The addition of an electron does not change the symmetry, but leads to an other strong peaks (at 1217 cm−1) in the high frequency region and redshifts the three main peaks from 1295, 262 and 143 cm−1 for B44 (I) to 1271, 241, and 45 cm−1 for B44− (I), respectively, which will be useful to identify the anionic B44− (I) and neutral B44 (I).
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