Chemistry Labs

Materials chemistry

Carbon nanotubes, graphene, 2D materials

Relate carbon bonding and dimensionality to the electronic, mechanical, and optical properties of nanotubes, graphene, and other atomically thin materials.

IntuitionOne carbon sheet, several dimensions

Imagine a hexagonal carbon net. Leave it flat and it is graphene; roll it into a cylinder and it is a nanotube. Curving or stacking changes which directions electrons and heat can travel.

The chiral vector (n,m) specifies how the hexagonal sheet is joined around the tube; ideal single-wall tubes are metallic or semiconducting depending on the indices.

SchoolStructure and bonding

Definition: Graphene

A single atomic layer of sp²-bonded carbon in a honeycomb lattice. The σ bonds form a strong in-plane framework; p orbitals form delocalized π bands.

Each carbon has three nearest neighbours. In ideal graphene, the π and π* bands meet at Dirac points, giving a zero-gap semimetal rather than an ordinary semiconductor.

Carbon architectures
StructureDimensionality / signature
Graphene2D; Dirac bands
Nanotube1D transport; chirality-dependent gap
Few-layer stackInterlayer coupling matters

Example: Classifying a nanotube

Solution

In the nearest-neighbour zone-folding picture, n−m divisible by 3 gives a band crossing and metallic behaviour. Curvature can open a small gap except in armchair tubes; real defects and interactions also modify this rule.

UndergraduateChirality and electronic structure

Ch=na1+ma2,qquadd=aπn2+nm+m2\mathbf C_h=n\mathbf a_1+m\mathbf a_2,\\qquad d=\frac{a}{\pi}\sqrt{n^2+nm+m^2}

The chiral vector closes the graphene lattice around the circumference. With graphene lattice constant a≈0.246 nm, the diameter follows from its magnitude; quantized circumferential wavevectors intersect the graphene dispersion and determine subbands.

AdvancedBeyond a single ideal layer

Substrate screening, strain, edges, disorder, adsorbates, and interlayer stacking all reshape spectra. Moiré superlattices in twisted bilayers can produce narrow bands and correlated phases, but twist-angle inhomogeneity and competing orders complicate interpretation.

ResearchResearch frontier

References

  • Helical Microtubules of Graphitic Carbon · S. Iijima, 1991
  • Electric Field Effect in Atomically Thin Carbon Films · K. S. Novoselov, A. K. Geim, S. V. Morozov, D. Jiang, Y. Zhang, S. V. Dubonos, I. V. Grigorieva, A. A. Firsov, 2004
  • The Electronic Properties of Graphene · A. H. Castro Neto, F. Guinea, N. M. R. Peres, K. S. Novoselov, A. K. Geim, 2009
  • Moiré Bands in Twisted Double-Layer Graphene · R. Bistritzer, A. H. MacDonald, 2011