Abstract
Thermoelectric materials constitute an alternative source of sustainable energy, harvested from waste heat. Bi2Te3 is the most utilized thermoelectric alloy. We show that it can be readily prepared in nanostructured form by arc-melting synthesis, yielding mechanically robust pellets of highly oriented polycrystals. This material has been characterized by neutron powder diffraction (NPD), scanning electron microscopy (SEM), and electronic and thermal transport measurements. A microscopic analysis from NPD data demonstrates a near-perfect stoichiometry of Bi2Te3 and a fair amount of anharmonicity of the chemical bonds. The as-grown material presents a metallic behavior, showing a record-low resistivity at 320 K of 2 μΩ m, which is advantageous for its performance as a thermoelectric material. SEM analysis shows a stacking of nanosized sheets, each of them presumably single-crystalline, with large surfaces perpendicular to the c crystallographic axis. This nanostructuration notably affects the thermoelectric properties, involving many surface boundaries that are responsible for large phonon scattering factors, yielding a thermal conductivity as low as 1.2 W m−1 K−1 around room temperature.
Highlights
Thermoelectric materials can convert temperature gradients, prominently those generated by waste heat, into useful electrical power [1, 2]
Thermoelectric properties are assessed in terms of the figure of merit, ZT, defined as ZT = S2σT/κ, where S accounts for the Seebeck coefficient, σ is the electrical conductivity, κ is the thermal conductivity, and T is the absolute average temperature
We report on a complete characterization including transport (Seebeck, electrical and thermal conductivity, and Hall effect) and crystal structure from neutron powder diffraction (NPD) data to assess the microscopic nature of the raw material
Summary
Thermoelectric materials can convert temperature gradients, prominently those generated by waste heat, into useful electrical power [1, 2]. Thermoelectric properties are assessed in terms of the figure of merit, ZT, defined as ZT = S2σT/κ, where S accounts for the Seebeck coefficient, σ is the electrical conductivity, κ is the thermal conductivity, and T is the absolute average temperature. Optimization of these physical properties is a challenging task as they depend on strongly correlated physical parameters.
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