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Potential Thermoelectric Performance from Optimization of Hole-Doped
Phys. Rev. X 1, 021005 – Published 31 October, 2011
DOI: https://doi.org/10.1103/PhysRevX.1.021005
Abstract
We present an analysis of the potential thermoelectric performance of hole-doped , which is commonly considered to show inferior room temperature performance when compared to . We find that if the lattice thermal conductivity can be reduced by nanostructuring techniques (as have been applied to in Refs. [W. Xie, X. Tang, Y. Yan, Q. Zhang, and T. M. Tritt, Unique Nanostructures and Enhanced Thermoelectric Performance of Melt-Spun BiSbTe Alloys, Appl. Phys. Lett. 94, 102111 (2009); B. Poudel et al., High-Thermoelectric Performance of Nanostructured Bismuth Antimony Telluride Bulk Alloys, Science 320, 634 (2008).]) the material may show optimized values of unity or more in the 300–500 K temperature range and thus be suitable for cooling and moderate temperature waste heat recovery and thermoelectric solar cell applications. Central to this conclusion are the larger band gap and the relatively heavier valence bands of .
Popular Summary
In the thermoelectric effect a voltage gradient is produced in a material due to the application of a thermal gradient. Thermoelectric performance relating to this effect is quantified by a single dimensionless parameter , with the best systems having a value of equal to about one or higher. Currently, the thermoelectric most in use is the narrow-band-gap semiconductor , with a approximately equal to one in a narrow temperature range around room temperature. The quest for better thermoelectrics has been a scientific challenge for the last fifty years, and systems with significantly higher than one are needed for applications. Here we theoretically investigate a related compound and show how its performance may be significantly improved.
The chalcogenide contains the same physical structure as , but has not generally been considered to be a useful thermoelectric due to its lower mobility. However, we find via first principles and Boltzmann transport calculations that its thermopower—voltage gradient per unit temperature gradient—is significantly higher than that of across the temperature range from 300 to 600 K. We further find that if this material is optimized, as has been done for , by optimizing carrier concentration, alloying, and nanostructuring, it may show comparable or better performance than , particularly at elevated temperatures. This is important because selenium is much more naturally abundant than tellurium, so that is more suitable for applications. Applications of thermoelectrics that have received considerable interest include electrical power generation from waste heat sources and ambient temperature refrigeration.
Article Text
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