Universal Limits of Thermopower and Figure of Merit from Transport Energy Statistics

Abstract

The search for new thermoelectric materials aims at improving their power and efficiency, as expressed by thermopower S and figure of merit ZT . By considering a very general transport spectral function W (E), expressions for S and ZT can be derived, which contain the statistical weights of an effective distribution function only, see Refs. [1][2][3] .We assumption of a Lorentzian shape with width k B T resulting from the electron-phonon coupling allows to estimate an upper limit of S and ZT independent on the microscopic mechanisms of the transport process. A simple estimate for an upper limit of the thermopwer S is derived from formula. It is given by 3 times the unit of the thermopower k b /e which is about 250 µV /K.We consider different systems which represent the general features of the electronic structure of thermoelectric relevant materials very well. The transport integrals were evaluated varying the band gap size and the chemical potential position. For all cases upper limits for both, the thermopower and the figure of merit, are obtained. The universal limit of |S| is given by 1.88 in units of k B /e, which is about 160 µV /K. The universal limit for ZT is obtained by about 1.11, which is in good agreement with available thermoelectric systems and devices.