Hübschle Christian B, Scheins Stephan, Weber Manuela, Luger Peter, Wagner Armin, Koritsánszky Tibor, Troyanov Sergey I, Boltalina Olga V, Goldt Il'ya V
Institut für Chemie und Biochemie/Kristallographie, Freie Universität Berlin, Fabeckstrasse 36a, 14195 Berlin, Germany.
Chemistry. 2007;13(7):1910-20. doi: 10.1002/chem.200601616.
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.
通过在20K下使用常规Mo(Kα)辐射对C60Cl30进行测量以及在92K下使用同步辐射对氟化合物进行测量所获得的高分辨率X射线数据集,确定了卤代C(60)富勒烯C(60)F(18)和C(60)Cl(30)的实验电荷密度。利用巴德的AIM理论分析了键拓扑和原子性质。对于长度在1.35至1.70 Å之间变化的不同C-C键,根据键临界点(BCP)处的键拓扑性质计算出键级n在n = 2至明显低于n = 1之间。对于每个贡献碳带有一个卤原子的5/6键,观察到低键级。通过在电子密度梯度矢量场中对巴德零通量盆地进行积分,也获得了原子性质。与所有碳原子具有11 ų的均匀体积且电荷为零的游离C(60)相反,卤代化合物中的原子体积大致在5至10 ų之间变化。在Cl衍生物中也发现几乎为零的原子电荷,但由于氟的电负性较高,在C(60)F(18)中C和F之间存在高达±0.8 e的电荷分离,这在静电势中也可见,碳和氟之间的电负性差异以及在富勒烯笼的一个半球上的附加导致沿着C(60)F(18)分子的强势梯度。从所有原子体积的总和可以看出,卤素的添加不仅导致C(60)笼的显著变形,还导致其体积的显著收缩。