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Charge and energy transport in graphene with smooth finite-range disorder
ref [60] · 2602.17453 · notice #8232 · dispute
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H. Sevinçli, C. Sevik, T. Ça ˘gın, G. Cuniberti, A bottom-up route to enhance thermoelectric figures of merit in graphene nanoribbons, Sci- entific Reports 3 (1) (2013) 1228.doi:10.1038/srep01228. URLhttps://doi.org/10.1038/srep01228 :Preprint submitted to Elsevier Page 10 of 10 0.0 0.2 0.4 0.6 0.8 1.0 0 10 20 30 40 50 60 (a) 0.0 0.2 0.4 0.6 0.8 1.0 0 10 20 30 40 50 60 (b) Figure 2:Transport relaxation time (in picoseconds) as a function of the Fermi energy, calculated using Eq.(18)for a random distribution of 3 nm-radius soft spheres with a concentration of𝑛 imp =1×10 12 cm−2, and for various poten- tials. The subfigure (a) corresponds to positive soft sphere potentials, whereas (b) corresponds to negative ones. -40 -20 0 20 40 0 100 200 300 400 500 600 (a) 2.5 3.0 3.5 4.0 4.5 5.00 100 200 300 400 500 600 700 (b) Figure 3:DC conductivity at zero temperature versus (a) the radii of the spheres and (b) the soft-sphere potential. In both cases, the Fermi energy isℰ 𝐹 =200meV. :Preprint submitted to Elsevier Page 11 of 10 0.0 0.2 0.4 0.6 0.8 1.00 2 4 6 8 10 12 14 (a) 0.0 0.2 0.4 0.6 0.8 1.00 1 2 3 4 5 (b) 0.0 0.2 0.4 0.6 0.8 1.00.0 0.5 1.0 1.5 (c) Figure 4:DC conductivity versus the F