It is always said that the Kohn anomaly of graphene is moved away from the gamma point, when graphene is doped.

I am confused about such discription. What will the phonon dispersion look like at that time (when doped)? Where is the Kohn anomaly moved to? Is the kink (Kohn anomaly) of the phonon dispersion curve smoothed or the kink moved to somewhere else?

ref:

'Doping changes the Fermi surface of graphene. This moves

the Kohn anomaly away from q = 0'

in 'Raman spectroscopy of graphene and graphite: Disorder, electron–phonon coupling, doping and nonadiabatic effects' by Prof. Andrea C.Ferrari

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