Max Planck Institute for Solid State Research, Heisenbergstr. 1, 70569 Stuttgart, Germany.
Chemistry. 2011 Feb 7;17(6):1798-805. doi: 10.1002/chem.201002731. Epub 2011 Jan 17.
A new fulleride, (K[DB18C6])(4)(C(60))(5)·12THF, was prepared in solution using the "break-and-seal" approach by reacting potassium, fullerene, and dibenzo[18]crown-6 in tetrahydrofuran. Single crystals were grown from solution by the modified "temperature difference method". X-ray analysis was performed revealing a reversible phase transition occurring on cooling. Three different crystal structures of the title compound at different temperatures of data acquisition are addressed in detail: the "high-temperature phase" at 225 K (C2, Z=2, a=49.055(1), b=15.075(3), c=18.312(4) Å, β=97.89(3)°), the "transitional phase" at 175 K (C2 m, Z=2, a=48.436(5), b=15.128(1), c=18.280(2) Å, β=97.90(1)°), and the "low-temperature phase" at 125 K (Cc, Z=4, a=56.239(1), b=15.112(3), c=36.425(7) Å, β=121.99(1)°). On cooling, partial radical recombination of C(60)(·-) into the (C(60))(2)(2-) dimeric dianion occurs; this is first time that the fully ordered dimer has been observed. Further cooling leads to formation of a superstructure with doubled cell volume in a different space group. Below 125 K, C(60) exists in the structure in three different bonding states: in the form of C(60)(·-) radical ions, (C(60))(2)(2-) dianions, and neutral C(60), this being without precedent in the fullerene chemistry, as well. Experimental observations of one conformation exclusively of the fullerene dimer in the crystal structure are further explained on the basis of DFT calculations considering charge distribution patterns. Temperature-dependent measurements of magnetic susceptibility at different magnetic fields confirm the phase transition occurring at about 220 K as observed crystallographically, and enable for unambiguous charge assignment to the different C(60) species in the title fulleride.
一种新的富勒烯化合物,(K[DB18C6])(4)(C(60))(5)·12THF,通过在四氢呋喃中反应钾、富勒烯和二苯并[18]冠-6 采用“打破-密封”方法在溶液中制备。通过改进的“温差法”从溶液中生长单晶。进行了 X 射线分析,揭示了冷却时发生的可逆相转变。详细讨论了标题化合物在不同温度下采集数据时的三种不同晶体结构:在 225 K 时的“高温相”(C2,Z=2,a=49.055(1),b=15.075(3),c=18.312(4)Å,β=97.89(3)°),在 175 K 时的“过渡相”(C2 m,Z=2,a=48.436(5),b=15.128(1),c=18.280(2)Å,β=97.90(1)°),以及在 125 K 时的“低温相”(Cc,Z=4,a=56.239(1),b=15.112(3),c=36.425(7)Å,β=121.99(1)°)。冷却时,C(60)(·-)部分重新组合成(C(60))(2)(2-)二聚二阴离子;这是首次观察到完全有序的二聚体。进一步冷却导致在不同空间群中形成具有两倍细胞体积的超结构。在 125 K 以下,C(60)以三种不同的键合状态存在于结构中:C(60)(·-)自由基离子、(C(60))(2)(2-)二阴离子和中性 C(60),这在富勒烯化学中是前所未有的。基于考虑电荷分布模式的 DFT 计算,进一步解释了晶体结构中仅观察到富勒烯二聚体一种构象的实验观察结果。在不同磁场下进行的磁化率随温度的测量证实了约 220 K 处发生的相转变,这与晶体学观察结果一致,并能够明确分配标题富勒烯中不同 C(60)物种的电荷。