2017
DOI: 10.1021/acsami.6b14266
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Understanding Phonon Scattering by Nanoprecipitates in Potassium-Doped Lead Chalcogenides

Abstract: We present a comprehensive experimental and theoretical study of phonon scattering by nanoprecipitates in potassium-doped PbTe, PbSe, and PbS. We highlight the role of the precipitate size distribution measured by microscopy, whose tuning allows for thermal conductivities lower than the limit achievable with a single size. The correlation between the size distribution and the contributions to thermal conductivity from phonons in different frequency ranges provides a physical basis to the experimentally measure… Show more

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Cited by 7 publications
(5 citation statements)
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“…In crystalline structures, Umklapp scattering dominates the phonon transport at the temperature range of interest, which shortens the phonon mean free path and leads to a reduction in the thermal conductivity with the temperature. The thermal conductivity of crystalline samples κ C is computed using the Callaway model 44 , which is expressed aswhere the average phonon relaxation time τ is computed combining phonon-grain boundary , film boundaries , phonon-impurity , Umklapp , phonon-carrier , and, in the case of Ag 3.9 Sb 33.6 Te 62.5 films, nanoprecipitate scattering mechanisms as 4547 , where D is the average grain size , P is the phonon transmission across the grain boundary, t is the thickness of the film, n NP is the nanoprecipitate number density, and Θ is the average nanoprecipitate scattering cross-section, which is estimated using the average nanoinclusion size, and the mass and tensor strength difference with the matrix 17,48 . As detailed at the beginning of this section, the thickness of the film is measured using cross-sectional SEM imaging and the grain size is derived from the XRD spectra.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…In crystalline structures, Umklapp scattering dominates the phonon transport at the temperature range of interest, which shortens the phonon mean free path and leads to a reduction in the thermal conductivity with the temperature. The thermal conductivity of crystalline samples κ C is computed using the Callaway model 44 , which is expressed aswhere the average phonon relaxation time τ is computed combining phonon-grain boundary , film boundaries , phonon-impurity , Umklapp , phonon-carrier , and, in the case of Ag 3.9 Sb 33.6 Te 62.5 films, nanoprecipitate scattering mechanisms as 4547 , where D is the average grain size , P is the phonon transmission across the grain boundary, t is the thickness of the film, n NP is the nanoprecipitate number density, and Θ is the average nanoprecipitate scattering cross-section, which is estimated using the average nanoinclusion size, and the mass and tensor strength difference with the matrix 17,48 . As detailed at the beginning of this section, the thickness of the film is measured using cross-sectional SEM imaging and the grain size is derived from the XRD spectra.…”
Section: Resultsmentioning
confidence: 99%
“…11 reached a zT of 1.4 at 550 K after doping AgSbTe 2 with 2% Se. Concentrations of silver lower than the stoichiometry can produce impurities in the matrix or form precipitates, both of which are favorable to reduce the thermal conductivity 17,18 . In particular, Sb 2 Te 3 /Ag 2 Te composites fabricated using ball milling have been found to improve the zT up to 1.5 at 700 K, and AgSbTe 2 /Ag 2 Te quenched ingots reached 1.5 at 500 K 19 .…”
Section: Introductionmentioning
confidence: 99%
“…For the NFO samples, we can estimate y by investigating which regime is more influential compared to the other, and thus closely examine t np À1 as follows. In the long-wavelength limit (w { 1), it has been shown [51][52][53] that mass density and force constant differences between nano-precipitates and host matrix play an important role in determining y. Our nano-NFO precipitates have almost identical structure and composition with those of the NFO matrix.…”
Section: View Article Onlinementioning
confidence: 85%
“…In addition, Bi nanoprecipitates can not only release the strain between the mismatched grains, but can also further promote charge redistribution as additional carriers, which are parallel to the result of modulated doping [21,22,165,166]. (PbQ, Q = Te, Se and S) thermoelectrics [13,14,164,168,169]. These nanostructures are thought to be inherent, which comes from the inevitable evaporation of lead during its formation process.…”
Section: Thermoelectrics: Structural Defect Engineering For Carrier and Phonon Transportmentioning
confidence: 99%
“…Such atomic-scale 2D planes of crystal mismatches densely pack together to form a 3D strain network, which is an effective scattering source for phonons with short to medium wavelengths. Furthermore, another type of planar defect, platelet-like precipitates with one/two atom-layer thickness, are characteristic nanostructures in lead chalcogenide (PbQ, Q = Te, Se and S) thermoelectrics [13,14,164,168,169]. These nanostructures are thought to be inherent, which comes from the inevitable evaporation of lead during its formation process.…”
Section: Thermoelectrics: Structural Defect Engineering For Carrier and Phonon Transportmentioning
confidence: 99%