“…At the same time, the low-energy phonon branches in the SWCNT differ significantly from the ones of graphite. For a quantitative description of these phonons we use a continuous model [49], which has been applied for the study of low-temperature specific heat of the carbon nanotubes [50]. Within this model the phonon state is determined with a 3 × 3 dynamic matrix, the structure of which depends on the phonon wave vector q and a discrete wave number n. During the intra-sub-band scattering process only the continuous electron wave vector is changed, while the discrete wave number along the circumference remains the same.…”