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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Zhang, Min
Royal Academy of Engineering
in Cooperation with on an Cooperation-Score of 37%
Topics
Publications (5/5 displayed)
- 2023Thermoelectric properties of Pnma and R3m GeS and GeSecitations
- 2020Expedient Synthesis of Heterobifunctional Triarylmethane Stoppers for Macromolecular Rotaxanescitations
- 2018Understanding and development of olivine LiCoPO4 cathode materials for lithium-ion batteriescitations
- 2015Fabrication of nanoporous copper surface by leaching of chill-zone Cu–Zr–Hf alloyscitations
- 2014Direct measurement of the vortex migration caused by traveling magnetic wavecitations
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article
Thermoelectric properties of Pnma and R3m GeS and GeSe
Abstract
With ∼60 % of global energy lost as heat, technologies such as thermoelectric generators (TEGs) are an important route to enhancing the efficiency of energy-intensive processes. Optimising ther- moelectric (TE) materials requires balancing a set of interdependent physical properties to meet efficiency, cost and sustainability requirements, and is a complex materials-design challenge. In this study, we demonstrate a fully first-principles modelling approach to calculating the properties and thermoelectric figure of merit ZT and apply it to the orthorhombic and rhombohedral phases of GeS and GeSe. We predict a large ZTmax = 2.12 for n-doped Pnma GeSe at 900 K, which would make it a good match for p-type SnSe in a thermoelectric couple. In contrast to the more usual p-type doping, the electrical conductivity σ is largest along the layering direction, which would combine with the low κlatt to produce a much larger ZTmax > 3 if the growth direction could be controlled. We also predict that p-doped R3m GeS and GeSe can achieve an industrially-viable ZT > 1, through a high σ counterbalanced by a large thermal conductivity, and experiments indicate this can be further improved by alloying. Our results therefore strongly motivate further study of the under-explored Ge chalcogenides as prospective TEs, with particular focus on strategies for n-doping the Pnma phases.