Abstract
The kinetic energy transport which is associated with the flow of free carriers in a semi-infinite spatially dispersive solid state plasma and which is induced by a TE polarised electromagnetic wave penetrating the surface at an oblique angle is considered. The angular splitting and the ratio between the magnitudes of the material and electromagnetic Poynting vectors are determined as functions of the frequency and the angle of incidence of the electromagnetic wave. Numerical calculations of the energy flow, based on near-local and fully non-local microscopic classical transport theories are presented for (far) infrared light in a heavily doped semiconductor (n-InSb) and (near) visible light in a metal (Al).
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