Abstract

One of the most popular routes used to improve the thermoelectric performance of materials is to suppress their lattice thermal conductivities. Thermoelectric performance is characterized by a figure-of-merit <i>zT</i>, which is defined as <i>σS<sup>2</sup>T</i>/(<i>κe</i> + <i>κl</i>), where the <i>σ</i>, <i>S</i>, <i>T</i>, <i>κe</i>, and <i>κl</i> are the electrical conductivity, Seebeck coefficient, temperature (in Kelvin), electronic thermal conductivity, and the lattice thermal conductivity, respectively. Among the variables in <i>zT</i>, the <i>κl</i> is the only variable that is independent of all other variables. In other words, reduction in <i>κl</i> guarantees <i>zT</i> improvement. Therefore, several different strategies to decrease <i>κl</i> have been introduced and implemented. Among the many <i>κl</i> reduction strategies, introducing point defects in the material by forming an alloy is particularly effective. Here, phonon scattering due to point defects in Mo(Se1-xTex)2 (<i>x</i> = 0.0, 0.25, 0.50, 0.75, 1.0) was studied using both the Debye-Callaway (DC) model and Callaway-von Baeyer (CvB) model. The advantages and disadvantages of using DC or CvB models are thoroughly discussed. When analyzing the effect of phonon scattering due to point defects, the CvB model is simpler and gives more information about the details of phonon scattering.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.