Right sizes of nano- and microstructures for high-performance and rigid bulk thermoelectrics

In this paper, we systematically investigate three different routes of synthesizing 2% Na-doped PbTe after melting the elements: (i) quenching followed by hot-pressing (QH), (ii) annealing followed by hot-pressing, and (iii) quenching and annealing followed by hot-pressing. We found that the thermoe...

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Published inProceedings of the National Academy of Sciences - PNAS Vol. 111; no. 30; pp. 10949 - 10954
Main Authors Wang, Hongchao, Bahk, Je-Hyeong, Kang, Chanyoung, Hwang, Junphil, Kim, Kangmin, Kim, Jungwon, Burke, Peter, Bowers, John E., Gossard, Arthur C., Shakouri, Ali, Kim, Woochul
Format Journal Article
LanguageEnglish
Published United States National Academy of Sciences 29.07.2014
National Acad Sciences
National Academy of Sciences, Washington, DC (United States)
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Summary:In this paper, we systematically investigate three different routes of synthesizing 2% Na-doped PbTe after melting the elements: (i) quenching followed by hot-pressing (QH), (ii) annealing followed by hot-pressing, and (iii) quenching and annealing followed by hot-pressing. We found that the thermoelectric figure of merit, zT , strongly depends on the synthesis condition and that its value can be enhanced to ∼2.0 at 773 K by optimizing the size distribution of the nanostructures in the material. Based on our theoretical analysis on both electron and thermal transport, this zT enhancement is attributed to the reduction of both the lattice and electronic thermal conductivities; the smallest sizes (2∼6 nm) of nanostructures in the QH sample are responsible for effectively scattering the wide range of phonon wavelengths to minimize the lattice thermal conductivity to ∼0.5 W/m K. The reduced electronic thermal conductivity associated with the suppressed electrical conductivity by nanostructures also helped reduce the total thermal conductivity. In addition to the high zT of the QH sample, the mechanical hardness is higher than the other samples by a factor of around 2 due to the smaller grain sizes. Overall, this paper suggests a guideline on how to achieve high zT and mechanical strength of a thermoelectric material by controlling nano- and microstructures of the material.
Bibliography:http://dx.doi.org/10.1073/pnas.1403601111
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USDOE Office of Science (SC), Basic Energy Sciences (BES) (SC-22)
SC0001009
Edited by Mildred S. Dresselhaus, Massachusetts Institute of Technology, Cambridge, MA, and approved June 13, 2014 (received for review February 26, 2014)
Author contributions: H.W. designed research; H.W., J.-H.B., C.K., J.H., K.K., J.K., P.B., and W.K. performed research; J.-H.B., J.E.B., A.C.G., A.S., and W.K. analyzed data; and H.W., J.-H.B., and W.K. wrote the paper.
ISSN:0027-8424
1091-6490
1091-6490
DOI:10.1073/pnas.1403601111