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C及其内嵌富勒烯衍生物在溶液态碳核磁共振谱中的精细结构。

Fine structure in the solution state C-NMR spectrum of C and its endofullerene derivatives.

作者信息

Bacanu George Razvan, Hoffman Gabriela, Amponsah Michael, Concistrè Maria, Whitby Richard J, Levitt Malcolm H

机构信息

Departament of Chemistry, University of Southmapton, Southampton SO17 1BJ, UK.

出版信息

Phys Chem Chem Phys. 2020 Jun 7;22(21):11850-11860. doi: 10.1039/d0cp01282c. Epub 2020 May 20.

DOI:10.1039/d0cp01282c
PMID:32432276
Abstract

The C NMR spectrum of fullerene C in solution displays two small "side peaks" on the shielding side of the main C peak, with integrated intensities of 1.63% and 0.81% of the main peak. The two side peaks are shifted by -12.6 ppb and -20.0 ppb with respect to the main peak. The side peaks are also observed in the C NMR spectra of endofullerenes, but with slightly different shifts relative to the main peak. We ascribe the small additional peaks to minor isotopomers of C containing two adjacent C nuclei. The shifts of the additional peaks are due to a secondary isotope shift of the C resonance caused by the substitution of a C neighbour by C. Two peaks are observed since the C structure contains two different classes of carbon-carbon bonds with different vibrational characteristics. The 2 : 1 ratio of the side peak intensities is consistent with the known structure of C. The origin and intensities of the C side peaks are discussed, together with an analysis of the C solution NMR spectrum of a C-enriched sample of C, which displays a relatively broad C NMR peak due to a statistical distribution of C isotopes. The spectrum of C-enriched C is analyzed by a Monte Carlo simulation technique, using a theorem for the second moment of the NMR spectrum generated by J-coupled spin clusters.

摘要

富勒烯(C)在溶液中的(^{13}C)核磁共振谱在主峰的屏蔽侧显示出两个小的“边峰”,其积分强度分别为主峰的(1.63%)和(0.81%)。这两个边峰相对于主峰分别位移了(-12.6) ppb和(-20.0) ppb。在内富勒烯的(^{13}C)核磁共振谱中也观察到了这些边峰,但相对于主峰的位移略有不同。我们将这些小的附加峰归因于含有两个相邻(^{13}C)核的(C)的次要同位素异构体。附加峰的位移是由于(^{13}C)共振的二次同位素位移,这是由一个(^{13}C)邻居被(^{12}C)取代引起的。观察到两个峰是因为(C)结构包含两类具有不同振动特征的碳 - 碳键。边峰强度的(2:1)比例与(C)的已知结构一致。讨论了(^{13}C)边峰的起源和强度,并对富含(^{13}C)的(C)样品的(^{13}C)溶液核磁共振谱进行了分析,由于(^{13}C)同位素的统计分布,该谱显示出相对较宽的(^{13}C)核磁共振峰。通过蒙特卡罗模拟技术对富含(^{13}C)的(C)的谱进行了分析,使用了由(J)耦合自旋簇产生的核磁共振谱的二阶矩定理。

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