Experimental and theoretical determination of the magnetic susceptibility of C60 and C70

THE magnetic susceptibility of C60 and the possibility of magnetic-field-induced π-electron ring currents in this carbon spheroid have been of interest since the initial experiments on carbon clusters1. If the molecule is regarded as a sphere with a radius of 3.5 Å, on which 60 electrons are free to move, the Pauling ring-current model predicts a ring-current diamagnetic susceptibility 41 times the π-electron ring-current magnetic susceptibility of benzene with the field normal to the plane of the six-membered ring2,3. London theory predicts, however, that the π-electron ring currents in C60 should be weakly paramagnetic or diamagnetic, depending on the relative bond strengths used in the calculation2,3. With the availability of macroscopic quantities of C60 (ref. 4), it is now possible to study experimentally the magnetic properties of the molecule. Here we report on such measurements. We find that the diamagnetism of C60 is small, a result that we attribute to excited-state paramagnetic contributions to the π-electron ring-current magnetic susceptibility. Thus C60 seems to be an aromatic molecule with a vanishingly small π-electron ring-current magnetic susceptibility. We have performed similar measurements on C70, which indicate an appreciable π-electron diamagnetism, consistent with theoretical calculations. We attribute the differences in magnetic properties of these two molecules to their different fractions of five-membered ring structures. The fullerenes may thus constitute a class of compounds of 'ambiguous' aromatic character, traditional measures of which will not provide an adequate classification.

[1]  Robert C. Haddon,et al.  Electronic structure and bonding in icosahedral C60 , 1986 .

[2]  W. Krätschmer,et al.  Solid C60: a new form of carbon , 1990, Nature.

[3]  Robert C. Haddon,et al.  .pi.-Electrons in three dimensiona , 1988 .

[4]  C. Coulson,et al.  Hückel theory for organic chemists , 1978 .

[5]  R. Haddon Geminal interactions at the termini of polyenes , 1977 .

[6]  R. Haddon,et al.  Solid-state magnetic resonance spectroscopy of fullerenes , 1991 .

[7]  Elser,et al.  Magnetic behavior of icosahedral Csub60. , 1987, Physical review. A, General physics.

[8]  Fred Wudl,et al.  Two different fullerenes have the same cyclic voltammetry , 1991 .

[9]  S. C. O'brien,et al.  C60: Buckminsterfullerene , 1985, Nature.

[10]  F. D. Salvo,et al.  Magnetic Susceptibility of Amorphous Semiconductors , 1972 .

[11]  R. Haddon The application of the Biot-Savart law to the ring current analysis of proton chemical shifts—II : An approach to aromatic character in the annulenes , 1972 .

[12]  T. Schmalz The magnetic susceptibility of Buckminsterfullerene , 1990 .

[13]  R. C. Haddon,et al.  Icosahedral C60: an aromatic molecule with a vanishingly small ring current magnetic susceptibility , 1987, Nature.

[14]  R. Haddon,et al.  Icosahedral C60 revisited: An aromatic molecule with a vanishingly small ring current magnetic susceptibility , 1990 .

[15]  Roberto Zanasi,et al.  Electric and magnetic properties of the aromatic sixty-carbon cage , 1990 .

[16]  R. Haddon,et al.  Naphtho[1,8-cd:4,5-c'd']bis[1,2,6]thiadiazine. A compound of ambiguous aromatic character , 1978 .

[17]  R. Haddon Unified theory of resonance energies, ring currents, and aromatic character in the (4n + 2).pi.-electron annulenes , 1979 .

[18]  R. Haddon,et al.  Large anisotropy and stage dependence of the magnetic susceptibility of alkali-graphite intercalation compounds , 1979 .

[19]  C. Coulson,et al.  Ring magnetic susceptibilities in conjugated hydrocarbons , 1975 .