Post-Processing Thermal Activation of Thermoelectric Materials Based on Germanium

After the deposition process, the lattice structure of doped germanium remains low. Post-processing annealing reorders the structure and increases the output parameters. Thin films of germanium doped with gold (Ge:Au) and vanadium (Ge:V) were magnetron-sputtered on glass substrates. The course of the activation process was monitored in situ. Two different methods of post-processing thermal activation of the films were studied. The first method was to place the structure at an elevated temperature for a specified period of time. The second method involved placing the structure on a heating table and cycling the heating and cooling several times from room temperature to about 823 K. Both methods fulfill their function well. The differences come down to research aspects. The best thermoelectric parameters were achieved for germanium doped with 0.95 at.% vanadium. The Seebeck coefficient of 212 μV/K and the power factor of 1.24 mW·m−1·K−2 were obtained at 500 K.

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Publication Details

Journal
Energies
Published
2024-12-27
DOI
https://doi.org/10.3390/en18010065
Primary Topic
Advanced Semiconductor Detectors and Materials
Type
article
Field-Weighted Citation Impact
0.00

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article

Post-Processing Thermal Activation of Thermoelectric Materials Based on Germanium

Piotr Markowski, Eugeniusz Prociów
Energies
Advanced Semiconductor Detectors and Materials
article

Post-Processing Thermal Activation of Thermoelectric Materials Based on Germanium

Piotr Markowski, Eugeniusz Prociów
article en

Abstract

After the deposition process, the lattice structure of doped germanium remains low. Post-processing annealing reorders the structure and increases the output parameters. Thin films of germanium doped with gold (Ge:Au) and vanadium (Ge:V) were magnetron-sputtered on glass substrates. The course of the activation process was monitored in situ. Two different methods of post-processing thermal activation of the films were studied. The first method was to place the structure at an elevated temperature for a specified period of time. The second method involved placing the structure on a heating table and cycling the heating and cooling several times from room temperature to about 823 K. Both methods fulfill their function well. The differences come down to research aspects. The best thermoelectric parameters were achieved for germanium doped with 0.95 at.% vanadium. The Seebeck coefficient of 212 μV/K and the power factor of 1.24 mW·m−1·K−2 were obtained at 500 K.

EnergiesVol. 18(1)
Wrocław University of Science and Technology (PL), AGH University of Krakow (PL)
Politechnika Wrocławska
Openalex Percentile: Top 78%
Advanced Semiconductor Detectors and Materials
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