The Limits of Thermoelectric Performance with a Bounded Transport Distribution

With the goal of maximizing the thermoelectric (TE) figure of merit $ZT$, Mahan and Sofo [Proc. Natl. Acad. Sci. U.S.A. 93, 7436 (1996)] found that the optimal transport distribution (TD) is a delta function. Materials, however, have TDs that appear to always be finite and non-diverging. Motivated by this observation, this study focuses on deriving what is the optimal bounded TD, which is determined to be a boxcar function for $ZT$ and a Heaviside function for power factor. From these optimal TDs upper limits on $ZT$ and power factor are obtained; the maximum $ZT$ scales with ${\mathrm{\Sigma }}_{\mathrm{m}\mathrm{a}\mathrm{x}}T\mathrm{/}{\kappa }_l$, where ${\mathrm{\Sigma }}_{\mathrm{m}\mathrm{a}\mathrm{x}}$ is the TD magnitude and ${\kappa }_l$ is the lattice thermal conductivity. These results help establish practical upper limits on the performance of TE materials and provide target TDs to guide band/scattering engineering strategies.