“…Thanks to the extremely thin thickness of only 0.34 nm, graphene can be regarded as an infinitely thin twodimensional planar material and ignores the edge effect. In the midst of this situation, the surface conductivity δ s (ω, µ c , , T ) based on the Kubo formula [18] are investigated to characterize the peculiar electronic properties of graphene. In general, δ s (ω, µ c , , T ) mainly consists two parts which are intraband contributions δ intra (ω, µ c , , T ) and interband contributions δ inter (ω, µ c , , T ), respectively, as shown in Eqs.…”