2009
DOI: 10.1007/s11664-009-0978-x
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Thermal Conductivity and Other Transport Properties of Mg2Sn:Ag Crystals

Abstract: The temperature dependence of the thermal conductivity j(T), electrical resistivity q(T), and Seebeck coefficient S(T) of Mg 2 Sn:Ag crystals with 0 at.% to 1 at.% Ag content were measured at T = 2 K to 400 K. The crystals were cut from ingots that were prepared by the vertical Bridgman method. Undoped samples show a dramatic j µ T 3 rise at low temperatures to a peak value j 15K = 477 W m À1 K À1 . This leads to exceptionally large phonon drag effects causing giant thermopower with S rising sharply to a peak … Show more

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Cited by 24 publications
(14 citation statements)
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“…It should be noted, however, that the PPMS apparatus tends to overestimate the thermal conductivity at temperatures above about 250 K [21]. As discussed previously [17,18] and observed here, the decrease in thermal conductivity with increasing addition of silver results from phonon scattering at point defects due to the substitutional silver atoms (i.e., at dopant sites) and by boundary scattering of phonons at the finely dispersed eutectic clusters and submicronsize Sn precipitates. It is noticeable, however, that the overlap of k data are very poor at higher silver contents ( Z0.3 at%).…”
Section: Thermoelectric Propertiessupporting
confidence: 58%
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“…It should be noted, however, that the PPMS apparatus tends to overestimate the thermal conductivity at temperatures above about 250 K [21]. As discussed previously [17,18] and observed here, the decrease in thermal conductivity with increasing addition of silver results from phonon scattering at point defects due to the substitutional silver atoms (i.e., at dopant sites) and by boundary scattering of phonons at the finely dispersed eutectic clusters and submicronsize Sn precipitates. It is noticeable, however, that the overlap of k data are very poor at higher silver contents ( Z0.3 at%).…”
Section: Thermoelectric Propertiessupporting
confidence: 58%
“…The carrier concentration was determined from Hall resistivity measurements using a PPMS apparatus (Physical Properties Measurement System, Quantum Design Inc.) on samples 1 Â 3 Â (8À 10) mm 3 cut adjacent to the samples used for the transport measurements. The thermal conductivity of RF samples was measured in the range 300-700 K using a laser flash apparatus (Netzsch LFA-427) [18], and is compared to that of the Bridgman samples using previously published data [17] in the range 2-400 K obtained using the PPMS.…”
Section: Characterization and Measurementsmentioning
confidence: 99%
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“…3b) and thus causes the observed enhancement of the power factor. Based on the thermal conductivity values presented in our companion paper 22 and the values measured above 300 K, 23 j = 4.5 W/m/K to 5 W/m/K at 400 K to 600 K for Mg 2 Sn samples doped with 1 at.% Ag, we estimate ZT max = 0.45 for sample 4B.…”
Section: Resultsmentioning
confidence: 85%