Transport in a biased lattice transitions from Landauer ballistic to Esaki-Tsu diffusive regime when Wannier-Stark localization length equals lattice length.
Notice that the lead capacity determines the electric field magnitude through the equation F = ∆µ CL
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Two-terminal transport in biased lattices: transition from ballistic to diffusive current
Transport in a biased lattice transitions from Landauer ballistic to Esaki-Tsu diffusive regime when Wannier-Stark localization length equals lattice length.