Institute of Problems of Chemical Physics RAS , Chernogolovka, Moscow region, 142432 Russia.
Inorg Chem. 2012 Mar 19;51(6):3420-6. doi: 10.1021/ic201732t. Epub 2012 Feb 29.
The salt (DMI(+))(2)·(C(60)(•-))·{Cd(Et(2)NCS(2))(2)I(-)} (1) containing fullerene radical anions, the anions of cadmium diethyldithiocarbamate iodide, and N,N'-dimethylimidazolium cations was obtained. Fullerenes are monomeric in 1 at 250 K and form three-dimensional packing in which each fullerene has nearly tetrahedral surroundings from neighboring fullerenes. Fullerenes with a shorter interfullerene center-to-center distance of 10.031(2) Å form spiral chains arranged along the lattice c axis. The convolution consists of four fullerene molecules. Dimerization realized in 1 within the spiral chains below 135 K manifests a strong dependence on the cooling rate. The "frozen" monomeric phase was obtained upon instant quenching of 1. This phase is stable below 95 K for a long time but slowly converted to the dimeric phase at T > 95 K. It exhibits a weak antiferromagnetic interaction of spins below 95 K (the Weiss temperature is -4 K), which results in the splitting of the electron paramagnetic resonance (EPR) signal into two components below 10 K. A disordered phase containing both C(60)(•-) monomers and singly bonded (C(60)(-))(2) dimers with approximately 0.5/0.5 occupancies is formed at an intermediate cooling rate (for 20 min). The position of each fullerene in this phase is split into three positions slightly shifted relative to each other. The central position corresponds to nonbonded fullerenes with interfullerene center-to-center distances of 9.94-10.00 Å. Two other positions are coincided to dimeric fullerenes formed with the right and left fullerene neighbors within the spiral chain. This intermediate phase is paramagnetic with nearly zero Weiss temperature due to isolation of C(60)(•-) by diamagnetic species and exhibits a strongly asymmetric EPR signal below 20 K. A diamagnetic phase containing ordered singly bonded (C(60)(-))(2) dimers can be obtained only upon slow cooling of the crystal for 6 h.
含有富勒烯自由基阴离子、二乙基二硫代氨基甲酸钠镉阴离子和 N,N'-二甲基咪唑阳离子的盐(DMI(+))(2)·(C(60)(•-))·{Cd(Et(2)NCS(2))(2)I(-)}(1)被获得。在 250K 时,富勒烯在 1 中为单体形式,并形成三维堆积,其中每个富勒烯具有来自相邻富勒烯的近乎四面体的环境。具有较短的富勒烯间中心到中心距离 10.031(2)Å 的富勒烯形成沿晶格 c 轴排列的螺旋链。卷积由四个富勒烯分子组成。在低于 135K 的螺旋链中实现的二聚化在冷却速率上表现出强烈的依赖性。通过对 1 的即时淬火获得“冻结”的单体相。该相在低于 95K 的温度下长时间稳定,但在 T > 95K 时缓慢转变为二聚相。它在低于 95K 时表现出自旋的弱反铁磁相互作用(魏斯温度为-4K),这导致电子顺磁共振(EPR)信号在低于 10K 时分裂成两个分量。在中间冷却速率(20 分钟)下形成包含 C(60)(•-)单体和单键合(C(60)(-))(2)二聚体的无序相,其占有率约为 0.5/0.5。在该相中,每个富勒烯的位置分裂为三个略微相对移动的位置。中心位置对应于具有 9.94-10.00Å 富勒烯间中心到中心距离的非键合富勒烯。另外两个位置与螺旋链内的右富勒烯和左富勒烯邻居形成的二聚体位置重合。由于抗磁性物质隔离 C(60)(•-),中间相具有几乎为零的魏斯温度,表现出强非对称 EPR 信号,低于 20K。仅通过对晶体缓慢冷却 6 小时才能获得含有有序单键合(C(60)(-))(2)二聚体的抗磁性相。