Effect of Transition to Impurity Continuum on Thermoelectric Properties of the Semiconductor $\left(\text{Bi}_{1-\mathrm{x}} \text{Sb}_{\mathrm{x}}\right)_{2} \text{Se}_{3}$ Solid Solutions

The dependences of thermoelectric parameters (the Seebeck coefficient <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$S$</tex>, electrical conductivity <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\sigma$</tex>, thermoelectric power factor <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$P$</tex>) and microhardness <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$H$</tex> on the composition of polycrystalline semiconducting (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\left.\text{Bi}_{1-\mathrm{x}} \mathbf{S b}_{\mathbf{x}}\right)_{2} \text{Se}_{3}$</tex> solid solutions (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$x=0-0.2$</tex>) were obtained at room temperature. It was shown that all measured parameters vary nonmonotonically, exhibiting two extrema in the range of composition <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$x=0-0.04$</tex>. At <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$x&gt;0.04$</tex>, the dependences become monotonic: <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$H$</tex> and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$S$</tex> increase, while <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\sigma$</tex> and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$P$</tex> decrease. We explain the observed behavior of thermoelectric characteristics and microhardness by the existence of a transition of percolation type to impurity continuum and subsequent selforganization processes taking place in a solid solution with the possible formation of complexes and infinite cluster passing through them.

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Published
2024-10-07
DOI
https://doi.org/10.1109/khpiweek61434.2024.10877954
Primary Topic
Advanced Thermoelectric Materials and Devices
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article

Effect of Transition to Impurity Continuum on Thermoelectric Properties of the Semiconductor $\left(\text{Bi}_{1-\mathrm{x}} \text{Sb}_{\mathrm{x}}\right)_{2} \text{Se}_{3}$ Solid Solutions

T. N. Shelest, Kateryna Martynova, S. I. Menshikova, A. V. Meriuts et al.
Advanced Thermoelectric Materials and Devices
article

Effect of Transition to Impurity Continuum on Thermoelectric Properties of the Semiconductor $\left(\text{Bi}_{1-\mathrm{x}} \text{Sb}_{\mathrm{x}}\right)_{2} \text{Se}_{3}$ Solid Solutions

T. N. Shelest, Kateryna Martynova, S. I. Menshikova, A. V. Meriuts, O. N. Nashchekina, Olena Rogachova
article en

Abstract

The dependences of thermoelectric parameters (the Seebeck coefficient <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$S$</tex>, electrical conductivity <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\sigma$</tex>, thermoelectric power factor <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$P$</tex>) and microhardness <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$H$</tex> on the composition of polycrystalline semiconducting (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\left.\text{Bi}_{1-\mathrm{x}} \mathbf{S b}_{\mathbf{x}}\right)_{2} \text{Se}_{3}$</tex> solid solutions (<tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$x=0-0.2$</tex>) were obtained at room temperature. It was shown that all measured parameters vary nonmonotonically, exhibiting two extrema in the range of composition <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$x=0-0.04$</tex>. At <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$x&gt;0.04$</tex>, the dependences become monotonic: <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$H$</tex> and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$S$</tex> increase, while <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$\sigma$</tex> and <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">$P$</tex> decrease. We explain the observed behavior of thermoelectric characteristics and microhardness by the existence of a transition of percolation type to impurity continuum and subsequent selforganization processes taking place in a solid solution with the possible formation of complexes and infinite cluster passing through them.

National Technical University "Kharkiv Polytechnic Institute" (UA)
Openalex Percentile: Top 83%
Advanced Thermoelectric Materials and Devices
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