首页> 外文期刊>Chemistry: A European journal >Magnetic Coupling and Optical Properties of the S_6-Dodecakis(trifluoromethyl)fullerene Radical Anions in the Layered Salt (PPN~+)[C_(60)(CF_3)_(12)~(·-)]
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Magnetic Coupling and Optical Properties of the S_6-Dodecakis(trifluoromethyl)fullerene Radical Anions in the Layered Salt (PPN~+)[C_(60)(CF_3)_(12)~(·-)]

机译:层状盐(PPN〜+)[C_(60)(CF_3)_(12)〜(·-)]中S_6-十二烷基(三氟甲基)富勒烯自由基阴离子的磁耦合和光学性质

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摘要

Poly(trifluoromethyl)fullerene S_6-C_(60)(CF_3)_(12) was reduced by sodium fluorenone ketyl in the presence of (PPN)CI (PPN = bis(triphenylphosphine)iminium) to afford the salt (PPN)[C_(60)(CF_3)_(12)] (1), which contains C_(60)(CF_3)_(12)~(-) radical anions. In the crystal structure of 1, C_(60)(CF_3)_(12)~(·-) layers alternate with the PPN~+ cations. There are short F···F contacts between C_(60)(CF_3)_(12)·- radical anions within the layers but no G···C contacts. DFT calculations revealed that the negative charge on C_(60)(CF_3)_(12)·- is distributed mainly between sp~2 carbon and fluorine atoms, whereas spin density is localized mainly on the fullerene-cage sp~2 carbon atoms. IR and UV/ Vis/NIR spectra in the solid state and solution showed characteristic changes relative to those of neutral S_6-C_(60)(CF_3)_(12) due to the formation of radical anions. The solid-state electronic spectrum of 1 exhibits a single broad band at 738 nm attributed to C_(60)(CF_3)_(12)~(·-). Crystals of 1 show a narrow EPR signal with g =2.0025 (?H= 0.45 mT) at 300 K. The temperature dependence of the integral intensity follows the Curie-Weiss law with a negative Weiss temperature of -11.8 K (30-300 K) indicating antiferro magnetic interaction of spins. This dependence was approximated by the Heisenberg model for one-dimensional chains of antiferro magnetically interacting spins with exchange interaction JKK_B=-9.1 K. It was assumed that magnetic interaction between the C_(60)(CF_3)_(12)~(·_) spins in the layers is mediated by short F…F contacts.
机译:在(PPN)Cl(PPN =双(三苯基膦)亚胺)存在下,用芴酮酮基钠还原聚三氟甲基富勒烯S_6-C_(60)(CF_3)_(12),得到盐(PPN)[C_ (60)(CF_3)_(12)](1),其中含有C_(60)(CF_3)_(12)〜(-)自由基阴离子。在1的晶体结构中,C_(60)(CF_3)_(12)〜(·-)层与PPN〜+阳离子交替排列。层内C_(60)(CF_3)_(12)-自由基阴离子之间的F···F接触短,但没有G··C的接触。 DFT计算表明,C_(60)(CF_3)_(12)·-的负电荷主要分布在sp〜2碳原子与氟原子之间,而自旋密度主要分布在富勒烯笼中的sp〜2碳原子上。固态和溶液中的IR和UV / Vis / NIR光谱显示由于自由基阴离子的形成,相对于中性S_6-C_(60)(CF_3)_(12)的特征变化。 1的固态电子光谱在738 nm处具有一个宽带,归因于C_(60)(CF_3)_(12)〜(·-)。 1晶体在300 K时显示出窄的EPR信号,g = 2.0025(?H = 0.45 mT)。积分强度的温度依赖性遵循居里-魏斯定律,负魏斯温度为-11.8 K(30-300 K) )表示自旋的反铁磁性相互作用。对于Heferenberg模型,一维反铁磁性相互作用的自旋链具有交换相互作用JKK_B = -9.1 K,这种依赖关系近似。假定C_(60)(CF_3)_(12)〜(·_ )层的自旋是由短F…F接触介导的。

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