Seminar Festkörper- und Grenzflächenphysik KOMET - experimentell
June 14, 2016 at 12:15 p.m. in Newton-Raum, Staudingerweg 9, 1. Stock, Raum 122 (Nebengebäude)Prof. Dr. Hans-Joachim Elmers
Institut für Physik, KOMET 5
elmers@uni-mainz.de
Prof. Dr. H. J. Elmers
The thermoelectric figure of merit provides information about the heat to electricity conversion efficiency. It is expressed by the dimensionless figure of merit ZT=S2σTκ-1 containing only material dependent parameters (S - Seebeck coefficient, σ - electrical conductivity, κ - thermal conductivity) and the average operation temperature T. The goal of our work is to reduce κ by phonon scattering at the superlattice (SL) interfaces and, therefore, enhance ZT.
For symmetric SLs (TiNiSn:HfNiSn ratio=1 and variable SL period) we observe a very good agreement between the cross-plane thermal conductivity measured by the 3ω method and a calculation based on Boltzmann transport theory, including a diffusive mismatch model for the phonons at the internal interfaces, down to a SL period of 3 nm. At the SL period of 3 nm a crossover between the particle- and the wave-like transport of phonons takes place and, therefore, κ increases for decreasing periods [1, 2].
The κ of non-symmetric SLs (constant period thickness = 6 unit cells, and variable material ratio (TiNiSn)n:(HfNiSn)6-n, with 0 ≤ n ≤ 6), shows a strong dependence on the material content achieving a minimum value for n=3. The measured κ can be well modeled using non-symmetric strain relaxation applied to the model of the series of thermal resistances. Additionally, a systematic improvement of the in-plane Seebeck coefficient in the non-symmetric sample series is observed [3].
References
[1] P. Hołuj, C. Euler, B. Balke, U. Kolb, G. Fiedler, M. M. Müller, T. Jaeger, E. Chávez Angel, P. Kratzer, and G. Jakob, Phys. Rev. B 2015, 92, 125436.
[2] P. Komar, T. Jaeger, C. Euler, E. Chávez Ángel, U. Kolb, M. M. Müller, B. Balke, M. H. Aguirre, S. Populoh, A. Weidenkaff, and Gerhard Jakob, Phys. Status Solidi A 2016, 213, 732–738.
[3] P. Komar, E. Chávez-Ángel, C. Euler, B. Balke, U. Kolb, M. M. Müller, H. J. Kleebe, G. H. Fecher, and G. Jakob, accepted to APL Materials