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Sn-Doping-Induced Biphasic Structure Advances Ductile AgS-Based Thermoelectrics. | LitMetric

Sn-Doping-Induced Biphasic Structure Advances Ductile AgS-Based Thermoelectrics.

Adv Sci (Weinh)

School of Chemistry and Physics, ARC Research Hub in Zero-emission Power Generation for Carbon Neutrality, and Centre for Materials Science, Queensland University of Technology, Brisbane, Queensland, 4000, Australia.

Published: November 2024

AI Article Synopsis

  • AgS, a flexible thermoelectric material, shows potential for harvesting waste heat but struggles with performance and maintaining ductility.
  • This study introduces a new method using Sn-doping to create a biphasic structure in AgSSe, which enhances both electron and phonon transport, achieving a promising thermoelectric figure-of-merit ZT of 0.42 while keeping ductility over 90%.
  • The biphasic structure effectively improves carrier mobility and reduces thermal conductivity, allowing the development of a flexible thermoelectric device with a high power density of roughly 49 µW cm under a temperature difference of 30 K, outperforming organic alternatives.

Article Abstract

Due to its inherent ductility, AgS shows promise as a flexible thermoelectric material for harnessing waste heat from diverse sources. However, its thermoelectric performance remains subpar, and existing enhancement strategies often compromise its ductility. In this study, a novel Sn-doping-induced biphasic structuring approach is introduced to synergistically control electron and phonon transport. Specifically, Sn-doping is incorporated into AgSSe to form a biphasic composition comprising (Ag, Sn)SSe as the primary phase and AgSSe as the secondary phase. This biphasic configuration achieves a competitive figure-of-merit ZT of 0.42 at 343 K while retaining exceptional ductility, exceeding 90%. The dominant (Ag, Sn)SSe phase bolsters the initially low carrier concentration, with interfacial boundaries between the phases effectively mitigating carrier scattering and promoting carrier mobility. Consequently, the optimized power factor reaches 5 µW cm K at 343 K. Additionally, the formation of the biphasic structure induces diverse micro/nano defects, suppressing lattice thermal conductivity to a commendable 0.18 W m K, thereby achieving optimized thermoelectric performance. As a result, a four-leg in-plane flexible thermoelectric device is fabricated, exhibiting a maximum power density of ≈49 µW cm under the temperature difference of 30 K, much higher than that of organic-based flexible thermoelectric devices.

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Source
http://www.ncbi.nlm.nih.gov/pmc/articles/PMC11578378PMC
http://dx.doi.org/10.1002/advs.202408374DOI Listing

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