Affiliation: | 1. College of Materials Science and Engineering, Nanjing Tech University, Nanjing, 210009 China;2. Centre for Future Materials, University of Southern Queensland, Springfield Central, Brisbane, Queensland, 4300 Australia Materials Engineering, The University of Queensland, Brisbane, Queensland, 4072 Australia;3. Materials Engineering, The University of Queensland, Brisbane, Queensland, 4072 Australia;4. School of Chemistry, Physics and Mechanical Engineering Faculty, Queensland University of Technology, Gardens Point Campus, Brisbane, Queensland, 4001 Australia;5. State Key Laboratory of Materials-Oriented Chemical Engineering, College of Chemical Engineering, Nanjing Tech University, Nanjing, 210009 China;6. Centre for Future Materials, University of Southern Queensland, Springfield Central, Brisbane, Queensland, 4300 Australia |
Abstract: | In this work, a record high thermoelectric figure-of-merit ZT of 1.6 ± 0.2 at 873 K in p-type polycrystalline Bi0.94Pb0.06CuSe1.01O0.99 by a synergy of rational band manipulation and novel nanostructural design is reported. First-principles density functional theory calculation results indicate that the density of state at the Fermi level that crosses the valence band can be significantly reduced and the measured optical bandgap can be enlarged from 0.70 to 0.74 eV by simply replacing 1% O with 1% Se, both indicating a potentially reduced carrier concentration and in turn, an improved carrier mobility and a boosted power factor up to 9.0 µW cm−1 K−2. Meanwhile, comprehensive characterizations reveal that under Se-rich condition, Cu2Se secondary microphases and significant lattice distortions triggered by Pb-doping and Se-substitution can be simultaneously achieved, contributing to a reduced lattice thermal conductivity of 0.4 W m−1 K−1. Furthermore, a unique shear exfoliation technique enables an effective grain refinement with higher anisotropy of the polycrystalline pellet, leading to a further improved power factor up to 10.9 µW cm−1 K−2 and a further reduced lattice thermal conductivity of 0.30 W m−1 K−1, which gives rise to record high ZT. |