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Contrasting Cu Roles Lead to High Ranged Thermoelectric Performance of PbS
Author(s) -
Qin Yongxin,
Hong Tao,
Qin Bingchao,
Wang Dongyang,
He Wenke,
Gao Xiang,
Xiao Yu,
Zhao LiDong
Publication year - 2021
Publication title -
advanced functional materials
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 6.069
H-Index - 322
eISSN - 1616-3028
pISSN - 1616-301X
DOI - 10.1002/adfm.202102185
Subject(s) - materials science , thermoelectric effect , atmospheric temperature range , phonon scattering , thermal conductivity , doping , microstructure , analytical chemistry (journal) , thermoelectric materials , phonon , lattice (music) , seebeck coefficient , electrical resistivity and conductivity , electron mobility , condensed matter physics , nanotechnology , thermodynamics , optoelectronics , metallurgy , composite material , electrical engineering , chemistry , physics , engineering , chromatography , acoustics
To obtain high‐performance PbS‐based thermoelectric materials, this study introduces Cu with different contrasting roles in p ‐type PbS, which can effectively decrease the lattice thermal conductivity and simultaneously optimize the electrical transport properties. Experimental results illustrate that Cu substitutions and Cu interstitials can improve carrier mobility through lowering effective mass ( m* ) and carrier concentration ( n H ) in a low temperature range (300–450 K), and further optimize temperature‐dependent n H in a high temperature range (450–823 K). Both decreased m* and n H shift the peak power factor to low temperature range, leading to an ultrahigh power factor ≈23 µW cm −1 K −2 at 423 K for Pb 0.99 Cu 0.01 S‐0.01Cu. Additionally, the special dynamic‐doping behaviors of Cu can continuously promote n H to approach the temperature‐dependent relationship of ( n H, opt ) ≈ ( m * T ) 1.5 , which brings about an eminent average power factor ( PF ave ) ≈ 18 µW cm −1 K −2 among 300–823 K in Pb 0.99 Cu 0.01 S‐0.01Cu. Furthermore, the microstructure characterizations unclose that the atomic and nanoscale Cu‐containing defects can effectively intensify the phonon scattering and suppress the lattice thermal conductivity. Consequently, both high ZT (≈0.2 at 300 K) and peak ZT (≈1.2 at 773 K) result in a record‐high average ZT ( ZT ave ) of ≈0.79 at 300–823 K for Pb 0.99 Cu 0.01 S‐0.01Cu.

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