As it is well known, carbon nanotubes may be one fold (Single Wall Carbon Nanotubes, SWCNT) or contain several cylinders nested one inside another (Multi Wall Carbon Nanotubes, MWCNT). SWCNT's, in many cases, self-organize into crystalline bundles (set of a few to a few hundred aligned tubes arranged in a two-dimensional triangular lattice in the plane perpendicular to their common axes).
A thorough understanding of carbon nanotubes (CNT's) includes the detailed and comprehensive characterization of their possible deformations due to interactions with a substrate or with other tubes, and their stability under thermal treatment or chemical agents.
In this communication we concentrate on i) the structural characteristics and ii) the structural transformations under thermal treatment of bundles of SWCNT's. i) Deformations of the tubes away from their ideal circular cross sections may have non trivial effects in their properties such as conductivity or phonon spectrum. We have being able to synthesize novel crystalline bundles of 'polygonized' SWCNT's. Our finding opens up the question of what is the equilibrium configuration of a lattice of aligned tubes and the possibility of the existence of several metastable structures which could be obtained depending on the growth conditions. To shed some light on this problem we have performed extensive molecular dynamics simulations of lattices of monodisperse armchair and zigzag SWCNT's as a function of tube diameter. We find several metastable structures of the lattice characterized by different tube cross sections, hexagonal, rounded-hexagonal and circular, and increasing cell volume. The competition between different tube shapes is analyzed and compared to experiments. ii) On the other hand, CNT's are metastable; (the most stable form of carbon is graphite). Due to their metastable character CNT's may transform into more stable structures under the appropriate annealing conditions. We have found that bundles of SWCNT's coalesce forming MWCNT's, containing from two to six nested tubes, under thermal treatment at high temperatures.
This structural transformation is confirmed by extensive Molecular Dynamics (MD) simulations. The simulations suggest a 'patching--and--tearing' mechanism for the SW-- to MWCNT's transformation underlying the 'concerted' coalescence of the tubes that begins with their polymerization. Tubes of different sizes and chiralities are considered.
Density functional theory is used to study the interaction of molecular and atomic hydrogen with (5,5) and (6,6) single wall carbon nanotubes. Molecular physisorption is predicted to be the most stable absorption state, with the molecule at a distance of 5-6 a.u. from the nanotube wall. The physisorption energies outside the nanutobes are about 0.07 eV, and twice as large inside. This means that uptake and release of molecular hydrogen from nanotubes is a relatively easy process, as many experiments have proved. A chemisorption state with the molecule dissociated has also been found, with the H atoms much closer to the nanotube wall. However, this dissociative state is separated from the physisorption state by an activation barrier of 2 eV or more. The dissociative chemisorption weakens C-C bonds, and the concerted effect of many incoming molecules with sufficient kinetic energies can lead to the scission of the nanotube.
Two recent experimental studies by Zweiback et al. and by Gobet et al. have motivated us to study the ground-state geometry and the consequent electronic structure of the singly-charged cationic hydrogen cluster H3+(H2)m for m=2,5 and 14, using at first the Hartree-Fock approximation. For the H+7 cluster the fully optimized ground-state geometry yeilds an isosceles triangle H3, with charge ~ 0.85(e), and sides 0.852 and 0.884 Å flanked by two H2 molecules lying parallel to each other, wiht bond lengths of 0.740 Å. In contrast, for the H+13 cluster, the central 'building block' is equilateral H3 with bond length 0.861 Å, and with charge ~0.815(e). This configuration of H3 is flanked by three almost-parallel H2 molecules with bond length 0.739 A. MP2 refinements of geometry, charge distribution and normal mode vibrational frequencies of the cationic tritium cluster T+7 and the corresponding deuterium cluster D+13 are also reported. Finally, Hartree-Fock and MP2 results are recorded for H+13.
We present ab initio calculations of phonons in single-wall boron nitride nanotubes. Raman and infrared active modes of isolated and infinitely long tubes are evaluated according to the non-symmorphic rod groups of BN nanotubes. For tubes of finite length, the selection rules are less restrictive and give rise to additional modes which may be observed in Raman and IR spectroscopy with an intensity depending on the tube length. Bundling of tubes is shown to have little effect on the phonon frequencies. However, arranging tubes in a large periodic array (larger than the wave-length of incoming light) gives rise to a strong frequency shift (LO-TO splitting) of some modes due to the establishing of a macroscopic electric field.
Modes of A1 symmetry experience a shift for laser light along the tube axis and E1 modes are split for light incidence in the perpendicular direction.
Conference Committee Involvement (2)
9 May 2005 | Sevilla, Spain
19 May 2003 | Maspalomas, Gran Canaria, Canary Islands, Spain