Artifacts in the Electron Paramagnetic Resonance Spectra of C60 Fullerene Ions: Inevitable C120O Impurity
Aspects of the electron paramagnetic resonance (EPR) spectra of C60 n - fulleride ions (n = 2, 3) and the EPR signal observed in solid C60 are reinterpreted. Insufficient levels of reduction and the unrecognized presence of C120O, a ubiquitous and unavoidable impurity in air-exposed C60, have compro...
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Published in | Journal of the American Chemical Society Vol. 124; no. 16; pp. 4394 - 4401 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
Washington, DC
American Chemical Society
24.04.2002
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Subjects | |
Online Access | Get full text |
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Summary: | Aspects of the electron paramagnetic resonance (EPR) spectra of C60 n - fulleride ions (n = 2, 3) and the EPR signal observed in solid C60 are reinterpreted. Insufficient levels of reduction and the unrecognized presence of C120O, a ubiquitous and unavoidable impurity in air-exposed C60, have compromised most previously reported spectra of fullerides. Central narrow line width signals (“spikes”) are ascribed to C120O n - (n = odd). Signals arising from axial triplets (g ∼ 2.0015, D = 26−29 G) in the spectrum of C60 2- are ascribed to C120O n - (n = 2 or 4). Their D values are more realistic for C120O than C60. Less distinct signals from “powder” triplets (D ∼ 11 G) are ascribed to aggregates of C120O n - (n = odd) arising from freezing nonglassing solvents. In highly purified samples of C60, we find no evidence for a broad ∼30 G signal previously assigned to a thermally accessible triplet of C60 2-. The C60 2- ion is EPR-silent. Signals previously ascribed to a quartet state of the C60 3- ion are ascribed to C120O4-. Uncomplicated, authentic spectra of C60 - and C60 3- become available when fully reduced samples are prepared under strictly anaerobic conditions from freshly HPLC-purified C60. Solid off-the-shelf C60 has an EPR signal (g ∼ 2.0025, ΔH pp ∼ 1.5 G) that is commonly ascribed to the radical cation C60 •+. This signal can be reproduced by exposing highly purified, EPR-silent C60 to oxygen in the dark. Doping C60 with an authentic C60 •+ salt gives a signal with much greater line width (ΔH pp = 6−8 G). It is suggested that the EPR signal in air-exposed samples of C60 arises from a peroxide-bridged diradical, •C60−O−O−C60 • or its decomposition products rather than from C60 •+. Solid-state C60 is more sensitive to oxygen than previously appreciated such that contamination with C120O is almost impossible to avoid. |
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Bibliography: | istex:9C2EBDF76F400253681492C572CFFF5A04AB1CB3 ark:/67375/TPS-XB6BZQFH-9 ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 0002-7863 1520-5126 |
DOI: | 10.1021/ja011832f |