Raman spectroscopy of small-diameter nanotubes

Results based on Raman measurements of small-diameter nanotubes (NTs) are presented and discussed in this paper. The NTs with diameters from 1 nm down to 0.4 nm were produced either as the inner tubes in the double-wall carbon NTs (DWCNTs) or as tubes embedded in the channels of the zeolite crystals. While analysing the Raman spectra attention was paid to the radial breathing mode (RBM), the D line and the G band. For both NT systems the RBM frequency was found to follow the same functional diameter dependence as the tubes with larger diameters. However, in contrast to the latter, the diameters of the thin tubes obtained from density functional theory calculations must be taken into account to explain satisfactorily the observed line positions. The resonance behaviour of the RBM intensities was recorded for the tubes in zeolites. It allows us to ascribe a position of the RBM to a particular NT. This result also demonstrates the breakdown of a simple tight-binding approach to the electronic structure but agrees with predictions from ab initio calculations. The D line of the outer tubes in DWCNTs is dispersive, similar to the single-wall carbon NTs. However, the rate of dispersion is reduced for the inner tubes in DWCNTs. This is attributed to the fact that the inner and outer tubes are probed with the same laser excitation. The linear shift due to the increasing laser energy is compensated by the negative shift due to the NT diameter. The latter is smaller for the inner NTs which leads to a stronger compensation of their dispersive behaviour. This effect is even stronger for the NTs in zeolites. In the extreme case, the strong Raman lines are not dispersive at all. This unexpected behaviour was explained by the detailed ab initio calculation of the phonon structure. The G bands of the inner semiconducting tubes were observed as new features in the Raman spectra of DWCNTs. On the other hand, no lines of metallic inner tubes were found. G bands of semiconducting as well as metallic NTs were detected for the zeolite samples. In either case, Raman lines due to the recently proposed Peierls-like mechanism for the thin metallic tubes were not indentified. This mechanism must therefore cause a significant reduction in Raman intensity.

[1]  H. Kataura,et al.  Determination of SWCNT diameters from the Raman response of the radial breathing mode , 2001 .

[2]  Daniel Sánchez-Portal,et al.  Ab initio calculations of the optical properties of 4-Å-diameter single-walled nanotubes , 2002 .

[3]  A. M. Rao,et al.  Large-scale purification of single-wall carbon nanotubes: process, product, and characterization , 1998 .

[4]  P. Eklund,et al.  Effect of the Growth Temperature on the Diameter Distribution and Chirality of Single-Wall Carbon Nanotubes , 1998 .

[5]  G. Kresse,et al.  Phonon softening in metallic nanotubes by a Peierls-like mechanism. , 2002, Physical review letters.

[6]  P. Eklund,et al.  Diameter-selective resonant Raman scattering in double-wall carbon nanotubes , 2002 .

[7]  C. T. Chan,et al.  Properties of 4 Å carbon nanotubes from first-principles calculations , 2002 .

[8]  Georg Kresse,et al.  Raman spectroscopy of template grown single wall carbon nanotubes in zeolite crystals , 2003 .

[9]  H. Kataura,et al.  Unusual high degree of unperturbed environment in the interior of single-wall carbon nanotubes. , 2003, Physical review letters.

[10]  H. J. Liu,et al.  Polarized absorption spectra of single-walled 4 A carbon nanotubes aligned in channels of an AlPO(4)-5 single crystal. , 2001, Physical review letters.

[11]  D. Vuillaume Electronic properties of molecular nanostructures , 2005 .

[12]  W. Krätschmer,et al.  High-yield fullerene encapsulation in single-wall carbon nanotubes , 2001 .

[13]  Bennett B. Goldberg,et al.  G-band resonant Raman study of 62 isolated single-wall carbon nanotubes , 2002 .

[14]  Zikang Tang,et al.  Mono-sized single-wall carbon nanotubes formed in channels of AlPO4-5 single crystal , 1998 .

[15]  Riichiro Saito,et al.  Origin of the Breit-Wigner-Fano lineshape of the tangential G-band feature of metallic carbon nanotubes , 2001 .

[16]  Thomsen,et al.  Double resonant raman scattering in graphite , 2000, Physical review letters.

[17]  M. Prato,et al.  A detailed Raman study on thin single-wall carbon nanotubes prepared by the HiPCO process , 2002 .

[18]  M. Hulman,et al.  Distribution of spectral moments for the radial breathing mode of single wall carbon nanotubes , 2001 .

[19]  F. Tuinstra,et al.  Raman Spectrum of Graphite , 1970 .

[20]  A. Grüneis,et al.  Double resonant raman phenomena enhanced by van Hove singularities in single-wall carbon nanotubes , 2002 .

[21]  V. Zólyomi,et al.  Assignment of chiral vectors in carbon nanotubes , 2003 .

[22]  Georg Kresse,et al.  Accurate density functional calculations for the phonon dispersion relations of graphite layer and carbon nanotubes , 2003 .

[23]  M. Dresselhaus,et al.  Stokes and anti-Stokes double resonance Raman scattering in two-dimensional graphite , 2002 .

[24]  M. Dresselhaus,et al.  Competing spring constant versus double resonance effects on the properties of dispersive modes in isolated single-wall carbon nanotubes , 2003 .