Xiangbin Chen, Tian Yu, Xiang Qu, Qixian Zheng, Ning Qi and Zhiquan Chen
{"title":"Optimization of the thermoelectric performance of Cu22Sn10S32-based composites†","authors":"Xiangbin Chen, Tian Yu, Xiang Qu, Qixian Zheng, Ning Qi and Zhiquan Chen","doi":"10.1039/D4NJ03811H","DOIUrl":null,"url":null,"abstract":"<p >Cu<small><sub>22</sub></small>Sn<small><sub>10</sub></small>S<small><sub>32</sub></small>, a type of Cu–Sn–S (CTS) compound, is known for its super-high carrier concentration, which is unfavorable for thermoelectric applications. In this work, nanostructured In<small><sub>2</sub></small>O<small><sub>3</sub></small> was incorporated into a Cu<small><sub>22</sub></small>Sn<small><sub>10</sub></small>S<small><sub>32</sub></small> matrix (CTS-<em>x</em> wt% In<small><sub>2</sub></small>O<small><sub>3</sub></small>, <em>x</em> = 0, 1, 2, 3, 4, 5, 6, 7) through high-energy ball milling in conjunction with spark plasma sintering. Microstructure analysis reveals that the introduced nano-In<small><sub>2</sub></small>O<small><sub>3</sub></small> reacts with Cu<small><sub>22</sub></small>Sn<small><sub>10</sub></small>S<small><sub>32</sub></small>, with In being uniformly doped in the matrix. At higher In<small><sub>2</sub></small>O<small><sub>3</sub></small> contents (<em>x</em> ≥ 5), a SnO<small><sub>2</sub></small> secondary phase appears. The incorporation of nano-In<small><sub>2</sub></small>O<small><sub>3</sub></small> leads to a substantial decrease in carrier concentration by one order of magnitude. At the same time, the carrier mobility shows a clear increase due to the suppressed carrier–carrier scattering. This ultimately lowers the electrical conductivity, which also contributes to a significant decrease in electronic thermal conductivity. Additionally, the lattice distortion caused by the substitution of In for Cu also leads to a significant reduction in lattice thermal conductivity. Ultimately, a maximum <em>zT</em> of 0.6 at 723 K was achieved for the CTS-5 wt% In<small><sub>2</sub></small>O<small><sub>3</sub></small> sample, which shows a 60% increase compared to the Cu<small><sub>22</sub></small>Sn<small><sub>10</sub></small>S<small><sub>32</sub></small> matrix. Our study illustrates that the introduction of nanoparticles into a CTS matrix can effectively lower its carrier concentration and lattice thermal conductivity, thereby optimizing its thermoelectric performance.</p>","PeriodicalId":95,"journal":{"name":"New Journal of Chemistry","volume":" 14","pages":" 5931-5939"},"PeriodicalIF":2.7000,"publicationDate":"2025-03-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"New Journal of Chemistry","FirstCategoryId":"92","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2025/nj/d4nj03811h","RegionNum":3,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Cu22Sn10S32, a type of Cu–Sn–S (CTS) compound, is known for its super-high carrier concentration, which is unfavorable for thermoelectric applications. In this work, nanostructured In2O3 was incorporated into a Cu22Sn10S32 matrix (CTS-x wt% In2O3, x = 0, 1, 2, 3, 4, 5, 6, 7) through high-energy ball milling in conjunction with spark plasma sintering. Microstructure analysis reveals that the introduced nano-In2O3 reacts with Cu22Sn10S32, with In being uniformly doped in the matrix. At higher In2O3 contents (x ≥ 5), a SnO2 secondary phase appears. The incorporation of nano-In2O3 leads to a substantial decrease in carrier concentration by one order of magnitude. At the same time, the carrier mobility shows a clear increase due to the suppressed carrier–carrier scattering. This ultimately lowers the electrical conductivity, which also contributes to a significant decrease in electronic thermal conductivity. Additionally, the lattice distortion caused by the substitution of In for Cu also leads to a significant reduction in lattice thermal conductivity. Ultimately, a maximum zT of 0.6 at 723 K was achieved for the CTS-5 wt% In2O3 sample, which shows a 60% increase compared to the Cu22Sn10S32 matrix. Our study illustrates that the introduction of nanoparticles into a CTS matrix can effectively lower its carrier concentration and lattice thermal conductivity, thereby optimizing its thermoelectric performance.