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Thermoelectric power factor in nanostructured materials with randomized nanoinclusions

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Figure

FIG. 1:(Colour online) The PF of a matrix material con-taining an 8 × 4 hexagonal array of nanoinclusions vs nanoin-clusion barrier height for two scattering regimes:Ballistic(coherent) transport (black-cross line), and acoustic phononscattering transport
FIG. 2:(Colour online) The materials with embedded NIsgeometries we consider: (a) The ordered structure consistingof 8 × 4 hexagonal array of NIs of barrier height VB = 0.05eV and diameter d = 3 nm
FIG. 3:(Colour online) Computational scheme for the self-consistent calculation
FIG. 4:(Colour online) The effect of variations of the NIdiameter and barrier height on the thermoelectric coefficients.(a) The electrical conductance, (b) the Seebeck coefficient,(c) the power factor, versus the percentage variation fromthe nominal values
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