31,389 research outputs found

    Carrier transport in 2D graphene layers

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    Carrier transport in gated 2D graphene monolayers is theoretically considered in the presence of scattering by random charged impurity centers with density nin_i. Excellent quantitative agreement is obtained (for carrier density n>1012cmβˆ’2n > 10^{12} \rm{cm}^{-2}) with existing experimental data (Ref. \onlinecite{kn:novoselov2004, kn:novoselov2005, kn:zhang2005, kn:kim2006, kn:fuhrer2006}). The conductivity scales linearly with n/nin/n_i in the theory, and shows extremely weak temperature dependence. The experimentally observed asymmetry between electron and hole conductivities is explained by the asymmetry in the charged impurity configuration in the presence of the gate voltage, while the high-density saturation of conductivity for the highest mobility samples is explained as a crossover between the long-range and the point scattering dominated regimes. We argue that the experimentally observed saturation of conductivity at low density arises from the charged impurity induced inhomogeneity in the graphene carrier density which becomes severe for n≲ni∼1012cmβˆ’2n \lesssim n_i \sim 10^{12} \rm{cm}^{-2}.Comment: 5 pages, 4 figures, published in Phys. Rev. Let

    Graphene magnetoresistance in a parallel magnetic field: Spin polarization effect

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    We develop a theory for graphene magnetotransport in the presence of carrier spin polarization as induced, for example, by the application of an in-plane magnetic field (BB) parallel to the 2D graphene layer. We predict a negative magnetoresistance ΟƒβˆB2\sigma \propto B^2 for intrinsic graphene, but for extrinsic graphene we find a non-monotonic magnetoresistance which is positive at lower magnetic fields (below the full spin-polarization) and negative at very high fields (above the full spin-polarization). The conductivity of the minority spin band (βˆ’)(-) electrons does not vanish as the minority carrier density (nβˆ’n_-) goes to zero. The residual conductivity of (βˆ’)(-) electrons at nβˆ’=0n_- = 0 is unique to graphene. We discuss experimental implications of our theory.Comment: 5 pages, 3 figure
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