The collective modes of coaxial-graphene-tubule systems are calculated
using both classical and quantum-mechanical approaches. While the der
ived results are valid for any number of coaxial tubules, the numerica
l results for the dispersion relations of the plasmons are presented f
or a system consisting of four graphene tubules for various values of
the azimuthal quantum number m. The lowest modes (m=0) are found to be
quasiacoustic, like the one-dimensional plasmons, whereas the higher
modes are of optical nature. For each m, the number of observable mode
s is equal to the number of tubules having a metallic character. The e
ffect of the intertubule interactions is a broadening of the frequency
range of the m modes. This broadening remains important so long as th
e plasmon momentum is significantly smaller than the Fermi momentum.