Resonance structures and aromaticity in capped carbon nanotubes
Source abstract
Abstract
Abstract The shape of a single-walled carbon nanotube’s cylinder is described by its chiral indices, (n,m), and important properties of the nanotube are determined by this pair of values. In particular, a nanotube is metallic or quasi-metallic when n-m is a multiple of 3, and is otherwise a semiconductor. This paper characterizes the conjugated π-systems that can form on capped nanotubes in each case. When n-m is a multiple of 3, there is a fully conjugated π-system running along the nanotube’s cylinder such that two-thirds of the hexagons are benzene rings and one-third are in a resonant set. In contrast, when n-m is not a multiple of 3, the pattern is broken along the length of the cylinder by two fracture lines. Surprisingly, and contrary to conventional thinking, these results are completely independent of the nanotube caps. The results are related to a similar characterization for open nanotubes by Ormsby and King, although in that case only a single fracture line is necessary. This new work is backed by the authors’ previous results on the Clar numbers of fullerenes in general. It also provides new predictions for nanotubes and introduces the concept of the aromaticity ratio.
Source: openaire · Quality: candidate unverified · Source record ↗
Research context
OpenAlex topics: Carbon Nanotubes in Composites · Fullerene Chemistry and Applications · Graphene research and applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (26)
Show source-provided references
1. Carbon nanotubes: present and future commercial applications10.1126/science.1222453 ↗
2. Carbon-nanotube photonics and optoelectronics10.1038/nphoton.2008.94 ↗
3. Nanoelectronics from the bottom up10.1038/nmat2028 ↗
4. Carbon nanotubes for electronic and electrochemical detection of biomolecules10.1002/adma.200700665 ↗
5. Fabrication of ultralong and electrically uniform single-walled carbon nanotubes on clean substrates10.1021/nl901260b ↗
6. Growth of half-meter long carbon nanotubes based on schulz-flory distribution10.1021/nn401995z ↗
7. A census of nanotube caps10.1016/S0009-2614(99)01111-2 ↗
8. A constructive enumeration of nanotube caps10.1016/S0166-218X(00)00328-0 ↗
9. Electronic structure of chiral graphene tubules10.1063/1.107080 ↗
10. Optical properties of single-wall carbon nanotubes10.1016/S0379-6779(98)00278-1 ↗
11. Clar valence bond representation of π-bonding in carbon nanotubes10.1021/jo035589+ ↗
12. Clar · 1972
13. Hartung · 2012
14. A pentagon-proximity model for local aromaticity in fullerenes and nanotubes10.1021/jp013642x ↗
15. Effect of nanotube length on aromaticity of single-wall carbon nanotubes10.1021/jp075742u ↗
16. Fullerenes with complete Clar structure10.1016/j.dam.2013.06.009 ↗
17. Clar chains and a counterexample10.1007/s10910-014-0305-5 ↗
18. The clar and fries structure of a fullerene I10.1016/j.dam.2016.07.016 ↗
19. Internal Kekule structures for graphene and general patches
20. Aromaticity of polycyclic conjugated hydrocarbons10.1021/cr9903656 ↗
21. Assessment of Clar’s aromatic pi-sextet rule by means of PDI, NICS, and HOMA indicators of local aromaticity10.1002/poc.938 ↗
22. Clar theory, pi-electron distribution, and geometry of graphene nanoribbons10.1021/ja909234y ↗
23. Clar theory extended for polyacenes and beyond10.1021/jp502235p ↗
24. Role of edges in the electronic and magnetic structures of nanographene10.1088/0031-8949/2012/T146/014008 ↗
25. Corso
26. Seligson