首页> 外文期刊>Journal of the American Chemical Society >Yb@C2n (n = 40, 41, 42): New Fullerene Allotropes with Unexplored Electrochemical Properties
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Yb@C2n (n = 40, 41, 42): New Fullerene Allotropes with Unexplored Electrochemical Properties

机译:Yb @ C2n(n = 40、41、42):具有未开发电化学特性的新型富勒烯同素异形体

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摘要

A series of13C-enriched monoytterbium endohedral metallofullerenes (EMFs)—Yb@C2n (n = 40, 41, 42)—was synthesized and isolated. Their cage structures were systematically determined for the first time using computational and experimental 13C NMR studies. The results revealed that all isomers adopt cage structures conforming to the isolated pentagon rule. In detail, Yb@C80 possesses the C2v(3) cage; Yb@C82(I, II, III) bear Cs(6), C2(5), and C2v(9) cages, respectively; and Yb@C84(II, III, IV) have C2(13), C1(12), and C2(11) cage structures, respectively. This is the first report describing C2(13)-C84 and C1(12)-C84 cage structures. It is noteworthy that the cage structures found for mono-EMFs generally differ from either the corresponding empty fullerenes or the related EMFs encapsulating more than one metal atom, indicating that the metal atom inside the fullerene cage plays an important role in determining the EMF structure. On the basis of the fact that the structure of Yb@C2(13)-C84 resembles that of Yb@C2(5)-C82, a metal-templated growth process was proposed as a kinetic factor controlling EMF formation. Furthermore, previous electrochemical studies of divalent EMFs have failed to observe their oxidation potentials, which have raised the assumption that such species are large-bandgap molecules. This study revealed that all isomers of Yb@C2n (n = 40, 41, 42) display one or two reversible oxidation steps together with four reversible reduction processes in 1,2-dichlorobenzene, even at a low scan rate (20 mV/s), which enables estimation of their electrochemical bandgaps (ΔE = oxE1 − redE1). The results show a ΔE value of 0.88−1.41 V for Yb@C2n (2n = 40, 41, 42), which is much larger than the values of trivalent mono-EMFs (ΔE < 0.5 V), but generally smaller than those of metal nitride cluster EMFs (1.4 V < ΔE < 2.1 V). Results further demonstrated that the ΔE values correlate reasonably with their relative abundances.
机译:合成并分离了一系列富含13 C的单面y金属内富勒烯(EMF)-Yb @ C2n(n = 40、41、42)。使用计算和实验13C NMR研究首次系统地确定了它们的笼结构。结果表明,所有异构体均采用符合孤立的五边形规则的笼状结构。具体地说,Yb @ C80具有C2v(3)笼; Yb @ C82(I,II,III)分别带有Cs(6),C2(5)和C2v(9)笼子; Yb @ C84(II,III,IV)分别具有C2(13),C1(12)和C2(11)笼状结构。这是描述C2(13)-C84和C1(12)-C84笼状结构的第一个报告。值得注意的是,发现单-EMF的笼结构通常不同于相应的空富勒烯或包封多个金属原子的相关EMF,这表明富勒烯笼内部的金属原子在确定EMF结构中起着重要作用。基于Yb @ C2(13)-C84的结构类似于Yb @ C2(5)-C82的事实,提出了金属模板生长过程作为控制EMF形成的动力学因子。此外,先前对二价EMF的电化学研究未能观察到它们的氧化电势,从而提出了这样的假设:此类物质是带隙大的分子。这项研究表明,即使在低扫描速率(20 mV / s)下,Yb @ C2n(n = 40、41、42)的所有异构体在1,2-二氯苯中也显示出一个或两个可逆氧化步骤以及四个可逆还原过程。 ),从而可以估算其电化学带隙(ΔE= oxE1-redE1)。结果显示Yb @ C2n的ΔE值为0.88-1.41 V(2n = 40、41、42),比三价单-EMF的值(ΔE<0.5 V)大得多,但通常小于金属氮化物簇EMF(1.4 V <ΔE<2.1 V)。结果进一步表明,ΔE值与其相对丰度合理相关。

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