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Theory of scattering of massive chiral fermions in bilayer graphene by radialsymmetric potential is developed. It is shown that in the case when theelectron wavelength is much larger than the radius of the potential thescattering cross-section is proportional to the electron wavelength. This leadsto the mobility independent on the electron concentration. In contrast with thecase of single-layer, neutral and charged defects are, in general, equallyrelevant for the resistivity of the bilayer graphene.

Scattering of charge carriers by point defects in bilayer graphene