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探索富勒烯与纳米管之间的界限:表征异构纯、空笼状和管状富勒烯-C和-C

Exploring the Threshold between Fullerenes and Nanotubes: Characterizing Isomerically Pure, Empty-Caged, and Tubular Fullerenes -C and -C.

作者信息

Schüßlbauer Christoph M, Krug Marcel, Ullrich Tobias, Franklin Hannah M, Stevenson Steven, Clark Timothy, Guldi Dirk M

机构信息

Department of Chemistry and Pharmacy & Interdisciplinary Center of Molecular Materials (ICMM), Friedrich-Alexander-Universität Erlangen-Nürnberg, Egerlandstraße 3, Erlangen 91058, Germany.

Department of Chemistry, Purdue University Fort Wayne, 2101 E. Coliseum Blvd, Fort Wayne, Indiana 46835, United States.

出版信息

J Am Chem Soc. 2022 Jun 22;144(24):10825-10829. doi: 10.1021/jacs.2c02442. Epub 2022 Jun 8.

Abstract

We report the fully fledged photophysical characterization of isomerically pure, empty-caged, tubular fullerenes -C and -C and compare their key properties. In particular, the focus was on cage sizes between 60 and 150 carbon atoms with , , and symmetry. The optical band gap of -C is 1.65 eV, which is larger than 1.37 eV of -C. In stark contrast to the nonluminescent -C, -C luminesces at room temperature. Transient absorption spectroscopy shows that photoexcited -C is subject to a slow intersystem crossing that generates a triplet excited state. In contrast, a fast, nonradiative internal conversion governs the deactivation of -C: In this case, exploring the corresponding triplet excited state required triplet-triplet sensitization experiments with anthracene. Density functional theory calculations revealed the electronic structure of the fullertubes, and calculations are consistent with our experimental findings. The calculated band gap systematically decreases with the number of carbon atoms within the and series. In contrast, an oscillating behavior is noted within the series of fullertubes. Finally, photoexcited -C was found to undergo hole transfer with electron-donating triethylamines readily but not electron transfer with electron-accepting methyl viologens.

摘要

我们报道了异构纯的、空笼状管状富勒烯-C和-C的完整光物理特性,并比较了它们的关键性质。特别地,重点关注了具有、和对称性、碳原子数在60到150之间的笼尺寸。-C的光学带隙为1.65 eV,大于-C的1.37 eV。与不发光的-C形成鲜明对比的是,-C在室温下发光。瞬态吸收光谱表明,光激发的-C会经历缓慢的系间窜越,从而产生三重激发态。相比之下,快速的非辐射内转换控制着-C的失活:在这种情况下,需要用蒽进行三重态-三重态敏化实验来探索相应的三重激发态。密度泛函理论计算揭示了富勒烯管的电子结构,计算结果与我们的实验发现一致。在和系列中,计算得到的带隙随着碳原子数的增加而系统地减小。相比之下,在系列富勒烯管中观察到振荡行为。最后发现,光激发的-C很容易与供电子的三乙胺发生空穴转移,但不与吸电子的甲基紫精发生电子转移。

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