Bond orders and atomic properties of the highly deformed halogenated fullerenes C60F18 and C60Cl30 derived from their charge densities |
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Authors: | Hübschle Christian B Scheins Stephan Weber Manuela Luger Peter Wagner Armin Koritsánszky Tibor Troyanov Sergey I Boltalina Olga V Goldt Il'ya V |
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Affiliation: | 1. Institut für Chemie und Biochemie/Kristallographie, Freie Universit?t Berlin, Fabeckstr. 36a, 14195 Berlin, Germany, Fax: (+49)?30‐8385‐3464;2. Paul Scherrer Institut, Swiss Light Source, WSLA/220, CH‐5232 Villigen PSI, Switzerland;3. Department of Chemistry, Middle Tennessee State University, P.O. Box 68, Murfreesboro, TN 37132, USA;4. Department of Chemistry, Moscow State University, 119992 Moscow, Leninskie Gory, Russia;5. Department of Chemistry, Colorado State University, Fort Collins, Colorado 80523, USA |
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Abstract: | The experimental charge densities of the halogenated C(60) fullerenes C(60)F(18) and C(60)Cl(30) were determined from high-resolution X-ray data sets measured with conventional Mo(Kalpha) radiation at 20 K for C(60)Cl(30) and with synchrotron radiation at 92 K for the fluorine compound. Bond topological and atomic properties were analyzed by using Bader's AIM theory. For the different C--C bonds, which vary in lengths between 1.35 and 1.70 A bond orders n between n=2 and significantly below n=1 were calculated from the bond topological properties at the bond critical points (BCP's). The low bond orders are seen for 5/6 bonds with each contributing carbon carrying a halogen atom. By integration over Bader's zero flux basins in the electron density gradient vector field atomic properties were also obtained. In contrast to free C(60), in which all carbon atoms have a uniform volume of 11 A(3) and zero charge, atomic volumes vary roughly between 5 and 10 A(3) in the halogenated compounds. Almost zero atomic charges are also found in the Cl derivative but a charge separation up to +/-0.8 e exists between C and F in C(60)F(18) due to the higher fluorine electronegativity, which is also seen in the electrostatic potential for which the electronegativity difference between carbon and fluorine, and the addition to one hemisphere of the fullerene cage leads to a strong potential gradient along the C(60)F(18) molecule. From the summation over all atomic volumes it follows that the halogen addition does not only lead to a dramatic distortion of the C(60) cage but also to a significant shrinkage of its volume. |
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Keywords: | bond order charge density fullerenes halogens topological analysis |
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