X-ray spectroscopic identification of strain and structure-based resonances in a series of saturated carbon-cage molecules: Adamantane, twistane, octahedrane, and cubane

T. Willey, Jonathan R. I. Lee, D. Brehmer, O. A. P. Mellone, L. Landt, P. Schreiner, A. Fokin, B. Tkachenko, A. Meijere, S. Kozhushkov, A. V. Buuren
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引用次数: 1

Abstract

Novel nanocarbons such as fullerenes, nanotubes, graphene, and nanodiamond reside at the cutting edge of nanoscience and technology. Along with chemical functionalization, geometric constraints (such as extreme curvature in nanotubes or defects within or at the surfaces of diamond nanoparticles) significantly alter the electronic states of the nanocarbon material. Understanding the effects of steric strain on the electronic structure is critical to developing nanoelectronic applications based on these materials. This paper presents a fundamental study of how strain affects the electronic structure in a benchmark series of some fundamental saturated carbon cage compounds. Adamantane, C10H16, the smallest diamondoid and arguably the smallest nanodiamond crystallite, has carbon atoms essentially commensurate with diamond lattice positions and possesses by far the least molecular strain of this series. Twistane also is a C10H16 isomer but the fixed cyclohexane twist conformation of the central ring introduces additional strain into the cage. Octahedrane [(CH)12] and cubane [(CH)8] are considerably more strained, culminating in cubane where carbon–carbon bonds lie either parallel or orthogonal to one another. Using gas-phase near-edge x-ray absorption fine structure spectroscopy to probe the unoccupied electronic states, we observe two major progressions across this series. First, a broad C–C σ* resonance in the absorption splits into two more narrow and intense resonances with increasing strain. Second, the first manifold of states previously associated with tertiary C–H σ* in the diamondoid series appears to broaden and shift to lower energy. This feature is more than twice as intense in cubane than in octahedrane, even though these two molecules have only tertiary carbons, with the chemical formula (CH)x. The spectral differences are entirely due to the shape of the molecules; in particular, in cubane, the features arise from a high degree of p-p interaction between parallel C–C bonds. In contrast to the conventional wisdom that near-edge x-ray absorption is primarily an atomically localized spectroscopy, molecular shape and associated strain lead to the dominant features in spectra acquired from this fundamental series of carbon cage structures.
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一系列饱和碳笼分子:金刚烷、扭烷、八面体烷和立方烷的应变和结构共振的x射线光谱鉴定
新型纳米碳,如富勒烯、纳米管、石墨烯和纳米金刚石,处于纳米科学和技术的前沿。随着化学功能化,几何约束(如纳米管的极端曲率或金刚石纳米颗粒内部或表面的缺陷)显着改变了纳米碳材料的电子状态。了解空间应变对电子结构的影响对于开发基于这些材料的纳米电子应用至关重要。本文介绍了应变如何影响一些基本饱和碳笼化合物基准系列的电子结构的基本研究。金刚烷C10H16是最小的类金刚石,也可以说是最小的纳米金刚石晶体,其碳原子与金刚石晶格位置基本一致,并且具有迄今为止该系列中最小的分子应变。Twistane也是C10H16异构体,但中心环的固定环己烷twist构象引入了额外的应变到笼中。八面体烷[(CH)12]和立方烷[(CH)8]的张力要大得多,在立方烷中达到顶点,碳-碳键彼此平行或正交。利用气相近边x射线吸收精细结构光谱来探测未占据电子态,我们观察到这一系列的两个主要进展。首先,随着应变的增加,吸收中的宽C-C σ*共振分裂成两个更窄和更强的共振。其次,金刚石系列中与叔碳-氢σ*相关的第一态流形似乎变宽并向低能量转移。尽管这两种分子只有叔碳,化学式为(CH)x,但立方烷的这种特性比八面体烷强两倍以上。光谱差异完全是由分子的形状造成的;特别是,在立方烷中,这些特征是由平行C-C键之间高度的p-p相互作用引起的。与传统观点相反,近边x射线吸收主要是原子局域光谱,分子形状和相关应变导致了从碳笼结构的基本系列中获得的光谱的主要特征。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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