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首页> 外文期刊>New Journal of Chemistry >Structure and magnetic properties of the ionic fullerene salt (TMP~+)·(Ceo~(·-)) C6H5CN containing layers of monomeric C_(60)~(·-) radical anions
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Structure and magnetic properties of the ionic fullerene salt (TMP~+)·(Ceo~(·-)) C6H5CN containing layers of monomeric C_(60)~(·-) radical anions

机译:离子性富勒烯盐(TMP〜+)·(Ceo〜(·-))C6H5CN单体C_(60)〜(·-)自由基阴离子层的结构和磁性

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摘要

The fullerene salt,(TMP~+)·(Ceo~(·-)) C6H5CN (1), with a layered structure was obtained as single crystals (TMP~+ is the N,N,N'-trimethylpiperazinium cation). The fullerene layers alternating with the TMP~+-C6H5CN layers along the c-axis have a honeycomb arrangement of C_(60)~(·-) in which each fullerene has three neighbors with interfullerene C···C contacts in the 3.13-3.38 A range. Despite the dense packing, the fullerene anions showed no intermolecular bond formation, even when down to helium temperatures. The structure of 1 was solved at 120 and 90 K. The fullerene molecules are disordered between three orientations at 120 K. The ordering transition observed in the 100-90 K range is accompanied by the trebling of the unit cell to provide three crystallographically independent fullerenes. The salt shows an asymmetric EPR signal down to 4 K which can be fitted by two Lorentzian lines with g1 = 1.9956 and a linewidth (ΔH) of 2.7 mT and g2 = 1.9815 and AH = 5.1 mT at room temperature. The ordering transition results in the abrupt narrowing of both lines in the 100-90 K range. The temperature dependence of the magnetic susceptibility of 1 follows the Curie-Weiss law with a negative Weiss temperature of -11 K, indicating an antiferromagnetic interaction of spins in the fullerene layers. Salt 1 is non-conducting with a room temperature resistivity of 7 × 107 ft cm, which is probably due to the orientational disorder of the fullerenes and a relatively weak interaction between C_(60)~(·-) in the layers, Indeed, the AM1 molecular orbital calculations show essentially smaller and more anisotropic overlap integrals between fullerenes than those in the layered metal (MDABCO~+)·(C_(60)~(·-))TPC.
机译:获得具有层状结构的富勒烯盐(TMP〜+)·(Ceo〜(·-))C6H5CN(1),为单晶(TMP〜+为N,N,N'-三甲基哌嗪鎓阳离子)。沿c轴与TMP〜+ -C6H5CN层交替的富勒烯层具有C_(60)〜(·-)的蜂窝排列,其中每个富勒烯具有3个邻域,在3.13中具有富勒烯间C···C接触。 3.38范围。尽管堆积密集,富勒烯阴离子仍未形成分子间键,即使在氦气温度下也是如此。 1的结构在120和90 K时分解。富勒烯分子在120 K时在三个方向之间无序。在100-90 K范围内观察到的有序跃迁伴随着晶胞的三倍转变,从而提供了三个晶体学上独立的富勒烯。盐显示低至4 K的非对称EPR信号,可在室温下由两条g1 = 1.9956,线宽(ΔH)为2.7 mT,g2 = 1.9815和AH = 5.1 mT的洛伦兹线拟合。有序过渡导致两条线在100-90 K范围内突然变窄。磁化率1的温度依赖性遵循居里-魏斯定律,负魏斯温度为-11 K,表明富勒烯层中自旋的反铁磁相互作用。盐1不导电,室温电阻率为7×107 ft cm,这可能是由于富勒烯的取向紊乱以及各层中C_(60)〜(·-)之间的相互作用相对较弱所致。 AM1分子轨道计算结果表明,与层状金属(MDABCO〜+)·(C_(60)〜(·-))TPC中的富勒烯相比,富勒烯之间的相互作用基本上更小且更各向异性。

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