Abstract

Icosahedral Al-Cu-Fe quasicrystal (QC) shows moderate electrical conductivity and low thermal conductivity, and both p- and n-type conduction can be controlled by tuning the sample composition, making it potentially suited for thermoelectric materials. In this work, we investigated the effect of introducing chemical disorder through heavy element substitution on the thermal conductivity of Al-Cu-Fe QC. We substituted Au and Pt elements for Cu up to 3 at% in a composition of Al63Cu25Fe12, i.e., Al63Cu25−x(Au,Pt)xFe12 (x = 0, 1, 2, 3). The substitutions of Au and Pt for Cu reduced the phonon thermal conductivity at 300 K (κph,300K) by up to 17%. The reduction of κph,300K is attributed to a decrease in the specific heat and phonon relaxation time through heavy element substitution. We found that increasing the Pt content reduced the specific heat at high temperatures, which may be caused by the locked state of phasons. The observed glass-like low values of κph,300K (0.9–1.1 W m−1 K−1 at 300 K) for Al63Cu25−x(Au,Pt)xFe12 are close to the lower limit calculated using the Cahill model.

Highlights

  • Academic Editors: Li-Dong Zhao and Lidong ChenReceived: 27 August 2021Accepted: 10 September 2021Published: 12 September 2021Thermoelectric materials can directly convert a temperature difference into electrical voltage

  • We focus on icosahedral Al-Cu-Fe QC for lowering κ t and investigate the effects of Au and

  • We found that the analyzed Au/Pt concentration increased with increasing nominal fraction, except for the sample of Al63 Cu22 Au3 Fe12, in which the secondary phase of Al2 Au was precipitated

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Summary

Introduction

Academic Editors: Li-Dong Zhao and Lidong Chen. Thermoelectric materials can directly convert a temperature difference into electrical voltage. Automotive exhaust, and industrial processes all generate enormous waste heat. Thermoelectric materials can recover waste heat emitted from commercial and industrial cycles. The potential of thermoelectric materials can be evaluated by the dimensionless figure of merit zT, as expressed by zT =. Publisher’s Note: MDPI stays neutral with regard to jurisdictional claims in published maps and institutional affiliations. T, κt where S, σ, κ t , and T are the Seebeck coefficient, the electrical conductivity, the total thermal conductivity, and the temperature, respectively [1,2]. Κ t is the sum of two contributions, the phonon part κ ph and the electron part κ el

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