Low-energy vibrations in Sc-2@C-84 and Tm@C-82 metallofullerenes with different carbon cages

Citation
M. Krause et al., Low-energy vibrations in Sc-2@C-84 and Tm@C-82 metallofullerenes with different carbon cages, J MOL STRUC, 521, 2000, pp. 325-340
Citations number
47
Categorie Soggetti
Physical Chemistry/Chemical Physics
Journal title
JOURNAL OF MOLECULAR STRUCTURE
ISSN journal
00222860 → ACNP
Volume
521
Year of publication
2000
Pages
325 - 340
Database
ISI
SICI code
0022-2860(20000328)521:<325:LVISAT>2.0.ZU;2-9
Abstract
Raman scattering and infrared absorption is reported for various empty and filled fullerene isomers in the low-energy range below 600 cm(-1) to clarif y the influence of different carbon cage structures on the bonding strength between encapsulated metal ion and fullerene cage and to check the potenti al of vibrational spectroscopy for isomer identification. The spectra of th ree isomers of Tm@C-82 and three isomers of SC2@C-84 were measured at room temperature. The results are compared to the response of the most abundant isomers of empty C-84 as well as to data for C-82 and C-60. The vibrational structure of the higher empty fullerene cages C-82 and C-84 resembles a downshifted and split C-60 spectrum. Moreover the spectra of t he two C-84 isomers exhibited only small differences due to the very simila r molecular structure, i.e. identical hexagon indices and direct neighbourh ood in the Stone-Wales conversion map. Larger differences of the low-energy cage modes were found for the Tm@C-82 isomers and in particular for the Sc -2@C-84 isomers. This goes along with an increasing difference in hexagon i ndices and a larger distance on the Stone-Wales conversion map. Due to the charge transfer from the endohedral metal to the fullerene the low-energy c age modes an shifted in the same direction as the modes of C-60 during the exohedral doping process with alkali metals. New lines induced by the endohedral scandium and thulium ions with almost c omplementary Raman and infrared intensities were found for Sc-2@C-84 below 200, around 250 and 260 cm(-1) and for Tm@C-82 at 116 to 118 cm(-1) and at 42 cm(-1). These vibrations were further identified as M-C-2n stretching an d M-C-2n deformation modes. Only a minor influence of the cage isomerism on these modes was observed. This is consistent with a simple ionic picture f or the interaction between carbon cage and encapsulated metal ion. It is th e amount of metal to fullerene charge transfer and the distance of the oppo sitely charge centres which determine the carbon cage-metal ion bond streng th. (C) 2000 Elsevier Science B.V. All rights reserved.