Please use this identifier to cite or link to this item: https://hdl.handle.net/10356/164587
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dc.contributor.authorWu, Mingen_US
dc.contributor.authorCui, Hong-Huaen_US
dc.contributor.authorCai, Songtingen_US
dc.contributor.authorHao, Shiqiangen_US
dc.contributor.authorLiu, Yukunen_US
dc.contributor.authorBailey, Trevor P.en_US
dc.contributor.authorZhang, Yinyingen_US
dc.contributor.authorChen, Zixuanen_US
dc.contributor.authorLuo, Yuboen_US
dc.contributor.authorUher, Ctiraden_US
dc.contributor.authorWolverton, Christopheren_US
dc.contributor.authorDravid, Vinayak P.en_US
dc.contributor.authorYu, Yanen_US
dc.contributor.authorLuo, Zhong-Zhenen_US
dc.contributor.authorZou, Zhigangen_US
dc.contributor.authorYan, Qingyuen_US
dc.contributor.authorKanatzidis, Mercouri G.en_US
dc.date.accessioned2023-02-06T02:26:55Z-
dc.date.available2023-02-06T02:26:55Z-
dc.date.issued2023-
dc.identifier.citationWu, M., Cui, H., Cai, S., Hao, S., Liu, Y., Bailey, T. P., Zhang, Y., Chen, Z., Luo, Y., Uher, C., Wolverton, C., Dravid, V. P., Yu, Y., Luo, Z., Zou, Z., Yan, Q. & Kanatzidis, M. G. (2023). Weak electron–phonon coupling and enhanced thermoelectric performance in n-type PbTe–Cu₂Se via dynamic phase conversion. Advanced Energy Materials, 13(1), 2203325-. https://dx.doi.org/10.1002/aenm.202203325en_US
dc.identifier.issn1614-6832en_US
dc.identifier.urihttps://hdl.handle.net/10356/164587-
dc.description.abstractThis study investigates Ga-doped n-type PbTe thermoelectric materials and the dynamic phase conversion process of the second phases via Cu2Se alloying. Introducing Cu2Se enhances its electrical transport properties while reducing its lattice thermal conductivity (κlat) via weak electron–phonon coupling. Cu2Te and CuGa(Te/Se)2 (tetragonal phase) nanocrystals precipitate during the alloying process, resulting in Te vacancies and interstitial Cu in the PbTe matrix. At room temperature, Te vacancies and interstitial Cu atoms serve as n-type dopants, increasing the carrier concentration and electrical conductivity from ≈1.18 × 1019 cm−3 and ≈1870 S cm−1 to ≈2.26 × 1019 cm−3 and ≈3029 S cm−1, respectively. With increasing temperature, the sample exhibits a dynamic change in Cu2Te content and the generation of a new phase of CuGa(Te/Se)2 (cubic phase), strengthening the phonon scattering and obtaining an ultralow κlat. Pb0.975Ga0.025Te-3%CuSe exhibits a maximum figure of merit of ≈1.63 at 823 K, making it promising for intermediate-temperature device applications.en_US
dc.description.sponsorshipAgency for Science, Technology and Research (A*STAR)en_US
dc.description.sponsorshipMinistry of Education (MOE)en_US
dc.language.isoenen_US
dc.relationRG128/21en_US
dc.relationA19D9a0096en_US
dc.relation.ispartofAdvanced Energy Materialsen_US
dc.rights© 2022 Wiley-VCH GmbH. All rights reserved. This is the peer reviewed version of the following article: Wu, M., Cui, H., Cai, S., Hao, S., Liu, Y., Bailey, T. P., Zhang, Y., Chen, Z., Luo, Y., Uher, C., Wolverton, C., Dravid, V. P., Yu, Y., Luo, Z., Zou, Z., Yan, Q. & Kanatzidis, M. G. (2023). Weak electron–phonon coupling and enhanced thermoelectric performance in n-type PbTe–Cu₂Se via dynamic phase conversion. Advanced Energy Materials, 13(1), 2203325-, which has been published in final form at https://doi.org/10.1002/aenm.202203325. This article may be used for non-commercial purposes in accordance with Wiley Terms and Conditions for Use of Self-Archived Versions.en_US
dc.subjectEngineering::Materialsen_US
dc.titleWeak electron–phonon coupling and enhanced thermoelectric performance in n-type PbTe–Cu₂Se via dynamic phase conversionen_US
dc.typeJournal Articleen
dc.contributor.schoolSchool of Materials Science and Engineeringen_US
dc.identifier.doi10.1002/aenm.202203325-
dc.description.versionSubmitted/Accepted versionen_US
dc.identifier.scopus2-s2.0-85141981296-
dc.identifier.issue1en_US
dc.identifier.volume13en_US
dc.identifier.spage2203325en_US
dc.subject.keywordsDynamic Phase Conversionen_US
dc.subject.keywordsElectron–Phonon Couplingen_US
dc.description.acknowledgementThis work was supported in part by the National Key Research and Development Program of China (No. 2020YFA0710303). At Northwestern work was supported in part by the Department of Energy, Office of Science, Basic Energy Sciences under Grant No. DE-SC0014520, (sample preparation, synthesis, XRD, TE measurements, TEM measurements, DFT calculations). This study was supported in part by the National Natural Science Foundation of China (Nos. 52102218, U1905215, and 52072076) and the Fujian Science & Technology Innovation Laboratory for Optoelectronic Information of China (No. 2021ZZ127). The authors acknowledge the Minjiang Scholar Professorship (GXRC-21004), the EPIC facility of Northwestern University's NUANCE Center, which received support from the Soft and Hybrid Nanotechnology Experimental (SHyNE) Resource (NSF ECCS-1542205), the MRSEC program (NSF DMR-1720139) at the Materials Research Center, International Institute for Nanotechnology (IIN), Keck Foundation, State of Illinois, through IIN, and the Office of Science of the U.S. Department of Energy under Contract Nos. DE-AC02-06CH11357 and DE-AC02-05CH11231. The high temperature Hall effect measurements made at the University of Michigan were supported by a grant from the U. S. Department of Energy (Grant No. DE-SC0018941). The authors also acknowledge the access to facilities for high-performance computational resources at Northwestern University and Singapore MOE AcRF Tier 1 RG128/21, Singapore A*STAR project A19D9a0096.en_US
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