Full metadata record
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Acharya, Somnath | - |
dc.contributor.author | Hwang, Junphil | - |
dc.contributor.author | Kim, Kwangrae | - |
dc.contributor.author | 김정원 | - |
dc.contributor.author | Hwang, Woohyun | - |
dc.contributor.author | Soon, Aloysius | - |
dc.contributor.author | Kim, Woochul | - |
dc.date.accessioned | 2024-01-12T06:35:25Z | - |
dc.date.available | 2024-01-12T06:35:25Z | - |
dc.date.created | 2023-05-09 | - |
dc.date.issued | 2023-07 | - |
dc.identifier.issn | 2211-2855 | - |
dc.identifier.uri | https://pubs.kist.re.kr/handle/201004/79893 | - |
dc.description.abstract | Here, we suggest that the quasi-random distribution of distorted nanostructures (QDDN), which is unique in high-entropy materials, is the reason for superior TE properties. The general high entropy material consists of several atoms with disordered lattice in atomic scale. Our QDDN showed nanoscale disorder because the consisting atoms were not distributed fully randomly. The order of compositional distribution was found as 40~60 nm, which causes high level of lattice-strain-induced distortion. The underlying mechanism of phonon scattering by QDDN was clarified by theoretical analysis. The high level of lattice strain induced by QDDN causes strong phonon scattering in entire phonon spectrum. A low κlat of ~0.38 W/m-K at 850 K was achieved in a CuGaTe2-based high-entropy chalcopyrite material. However, the power factor was not significantly affected due to the high crystallinity, despite the QDDN. Therefore, a zT of ~1.56 at 850 K was attained in a Cu0.8Ag0.2[Ga0.8In0.2]0.99Zn0.01Te2 compound, which represented a 132% enhancement from pure CuGaTe2. These results elucidate recent zT increases in high-entropy materials and can be a step towards further enhancements of zT in materials. | - |
dc.language | English | - |
dc.publisher | Elsevier BV | - |
dc.title | Quasi-random distribution of distorted nanostructures enhances thermoelectric performance of high-entropy chalcopyrite | - |
dc.type | Article | - |
dc.identifier.doi | 10.1016/j.nanoen.2023.108493 | - |
dc.description.journalClass | 1 | - |
dc.identifier.bibliographicCitation | Nano Energy, v.112 | - |
dc.citation.title | Nano Energy | - |
dc.citation.volume | 112 | - |
dc.description.isOpenAccess | N | - |
dc.description.journalRegisteredClass | scie | - |
dc.description.journalRegisteredClass | scopus | - |
dc.identifier.wosid | 001009137200001 | - |
dc.relation.journalWebOfScienceCategory | Chemistry, Physical | - |
dc.relation.journalWebOfScienceCategory | Nanoscience & Nanotechnology | - |
dc.relation.journalWebOfScienceCategory | Materials Science, Multidisciplinary | - |
dc.relation.journalWebOfScienceCategory | Physics, Applied | - |
dc.relation.journalResearchArea | Chemistry | - |
dc.relation.journalResearchArea | Science & Technology - Other Topics | - |
dc.relation.journalResearchArea | Materials Science | - |
dc.relation.journalResearchArea | Physics | - |
dc.type.docType | Article | - |
dc.subject.keywordPlus | ULTRALOW THERMAL-CONDUCTIVITY | - |
dc.subject.keywordPlus | TOTAL-ENERGY CALCULATIONS | - |
dc.subject.keywordPlus | POWER-FACTOR | - |
dc.subject.keywordPlus | CUINTE2 | - |
dc.subject.keywordAuthor | Thermoelectric | - |
dc.subject.keywordAuthor | High-entropy | - |
dc.subject.keywordAuthor | Nanostructures | - |
dc.subject.keywordAuthor | Lattice thermal conductivity | - |
dc.subject.keywordAuthor | Lattice strain | - |
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