Abstract

The calculation of Sondheimer on the galvanomagnetic effects in thin metallic films is extended so as to permit the evaluation of the Nernst, Ettinghausen, and Leduc-Righi coefficients (${A}_{N}, {A}_{E}, {A}_{L}$). It is assumed that the conduction electrons are quasi-free and that a relaxation time exists. General expressions are derived for ${A}_{N}$, ${A}_{E}$, and ${A}_{L}$ and the asymptotic forms are given in the limit of the ratio of film thickness to mean free path much less than unity. As this ratio approaches zero, ${A}_{N}$ and ${A}_{L}$ vanish whereas ${A}_{E}$ becomes infinite.

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