4.8 Article

Effects of Co-doping and Microstructure on Charge Carrier Energy Filtering in Thermoelectric Titanium-Doped Zinc Aluminum Oxide

Journal

ACS APPLIED MATERIALS & INTERFACES
Volume 14, Issue 3, Pages 4035-4050

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acsami.1c20300

Keywords

thermoelectric materials; electron and phonon transport; charge carrier energy filtering; zinc oxide; multiphase oxides

Funding

  1. Israel Science Foundation (ISF) [1997/18]
  2. Carl E. Shustak Energy Research and Development Fund at Technion-Israel Institute of Technology
  3. Israeli Ministry of Immigrant Absorption
  4. Technion Israel Institute of Technology

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In this study, Al and Ti co-doped ZnO with second and third phases were synthesized to enhance its power factor and unusual behavior was observed. By co-doping and employing a multiphase structure, the thermoelectric figure of merit was significantly increased.
ZnO is a promising thermoelectric (TE) material for high-temperature applications; however, its TE performance is limited by strong coupling between electrical and thermal transport. In this study, we synthesized Al and Ti co-doped ZnO by a solid-state reaction and air sintering at 1500 degrees C and analyzed the microstructure to establish its correlation with TE properties. The TE transport properties were measured between room temperature and 800 degrees C, and electronic properties were calculated from first principles calculations. Herein, we introduced second and third phases into a ZnO-based matrix to enhance its power factor (PF) by charge carrier energy filtering by applying co-doping with Al and Ti. Although multiphase materials usually do not exhibit high PF, in this study, it is observed that three-phase ZnO-based materials exhibit higher PF values compared to the two-phase materials. We observed unusual behavior, in which the Seebeck coefficient (S) and electrical conductivity (s) values increased simultaneously with temperature for Zn1-x-yAlxTiyO, originating from energy filtering of charge carriers due to both co-doping and the peculiar multiphase structure. High s values were associated with the increase of electron concentration, while high S values were due to Fermi energy tuning and heavier effective masses initiated by Al and Ti co-doping. Besides increasing the PF, the multiphase structure played an essential role in reducing lattice thermal conductivity due to phonon scattering by the Umklapp, point defect, and second-phase mechanisms. Our approach yielded an increase of the TE figure of merit upon formation of a three-phase 2 wt % Ti-doped Zn0.98Al0.02O compound of ca. 10 times compared to the corresponding value attained for its two-phase ZnAl0.02O counterpart.

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