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Fig. 3.20 FWHM of the
plasmon peak as a function of
a the parallel momentum
transfer q || and of b the
plasmon energy. The inset in
the top panel shows the origin
of interband SPEs from π to
π bands. The Fermi wave
vector represents the onset
where plasmon enters the
damping region
3.4.3
Dispersion and Damping Processes of
π
Plasmon
The electronic response of graphene systems is related to the collective excitations
of the electrons which combine in-plane and inter-plane interactions. Herein we
want to investigate the nature and the dispersion of
π
plasmon in MLG grown on a
metal substrate. The
plasmon is a sensitive probe of the graphene band structure
near the Fermi level (Sun et al. 2010 ). Its physical origin is the electric dipole
transition between the
π
π
energy bands (
π → π
*) mainly in the region of the M
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