2022
DOI: 10.1039/d1ta10711a
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Regulation of Ge vacancies through Sm doping resulting in superior thermoelectric performance in GeTe

Abstract: A high thermoelectric figure of merit ZT of 2.5 at 730 K is achieved in p-type Ge1−xSmxTe through synergetic optimization of electrical and thermal transport properties. Sm doping effectively suppresses...

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Cited by 24 publications
(27 citation statements)
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“…The τ ave is obtained by the formula τ ave = τ 1 I 1 + τ 2 I 2 (where I 1 + I 2 = 100%), which agrees well with the center of mass of the lifetime spectrum. Therefore, average lifetime τ ave behaves trustworthily to the uncertainties in the decomposition of the lifetime spectrum and is more dependable to characterize the vacancy defects’ properties . As shown in Table , the average positron lifetime (τ ave ) increases gradually from 258.6 ps for Pb 0.98 Na 0.02 Se to 287.3 ps for the x = 0.04 sample, and beyond that it gets saturated.…”
Section: Resultsmentioning
confidence: 87%
See 1 more Smart Citation
“…The τ ave is obtained by the formula τ ave = τ 1 I 1 + τ 2 I 2 (where I 1 + I 2 = 100%), which agrees well with the center of mass of the lifetime spectrum. Therefore, average lifetime τ ave behaves trustworthily to the uncertainties in the decomposition of the lifetime spectrum and is more dependable to characterize the vacancy defects’ properties . As shown in Table , the average positron lifetime (τ ave ) increases gradually from 258.6 ps for Pb 0.98 Na 0.02 Se to 287.3 ps for the x = 0.04 sample, and beyond that it gets saturated.…”
Section: Resultsmentioning
confidence: 87%
“…Therefore, average lifetime τ ave behaves trustworthily to the uncertainties in the decomposition of the lifetime spectrum and is more dependable to characterize the vacancy defects' properties. 38 As shown in Table 2, the average positron lifetime (τ ave ) increases gradually from 258.6 ps for Pb 0.98 Na 0.02 Se to 287.3 ps for the x = 0.04 sample, and beyond that it gets saturated. This indicates the growing population of cation vacancies with increasing Sn content and validates the above conjecture.…”
Section: Defect Chemistry Of Pb 098−x Snmentioning
confidence: 87%
“…After deducting source and background components, all lifetime spectra can be decomposed into two-lifetime components τ 1 and τ 2 by PATFIT software. The τ 1 and τ 2 are decided by the positron lifetime in a perfect PbSe lattice and in the defect trapping state (vacancies or dislocation), respectively. , I 1 and I 2 stand for corresponding intensities of τ 1 and τ 2 , respectively. All positron lifetime results are summarized in Table .…”
Section: Resultsmentioning
confidence: 99%
“…A large amount of V Sn acceptors lead to the ultra-high hole carrier concentration and the small thermopower as well as the large κ c , which inhibit the improvement of its ZT value; thus, the most common strategy of improving SnTe thermoelectric properties is to reduce the high carrier concentration. , In PbTe and GeTe , systems, the intrinsic defects are Pb and Ge vacancies, which would scatter charge carriers. Hence, many research studies tried to inhibit the cation vacancies by increasing the cation content or introducing extrinsic dopants to improve the μ. Because the intrinsic defects in Cu-containing chalcogenides CuInS 2 and Cu 2 ZnSnS 4 are V Cu and Cu Zn antisite, we speculate that the intrinsic point defects in Cu 2 SnSe 3 are V Cu and/or Cu Sn antisite defects. Whereas Cu–Se bonds form a hole conduction network in Cu 2 SnSe 3 , V Cu would damage the carrier conduction paths and scatter the charge carrier drastically.…”
Section: Introductionmentioning
confidence: 99%