Gabi Schierning1,Sepideh Izadi1,Sarah Salloum2,Ahana Bhattacharya2,Jeong Han2,Lauritz Schnatmann1,Stephan Schulz2,Martin Mittendorff2
Bielefeld University1,University of Duisburg-Essen2
Gabi Schierning1,Sepideh Izadi1,Sarah Salloum2,Ahana Bhattacharya2,Jeong Han2,Lauritz Schnatmann1,Stephan Schulz2,Martin Mittendorff2
Bielefeld University1,University of Duisburg-Essen2
Bismuth telluride is an excellent thermoelectric material and also belongs to the class of three-dimensional topological insulators. Therefore, surface charge carriers with extremely high mobility exist at the crystal surfaces. This is particularly visible in nanoparticulate samples, provided that the nanoparticles used have sufficient surface purity. Compacted nanoparticulate bulk samples exhibit a high density of interfaces. These samples show a pronounced weak anti-localization in the low-temperature transport behavior as well as a kink in the electrical resistance at about 5 K. Evaluation of the magnetotransport data using the Hikami-Larkin-Nagaoka model yields coherence lengths of up to 200 nm, which is significantly larger than the average grain size in the studied samples. Using terahertz spectroscopy, the average mobility of the surface charge carriers can be estimated to be about 1000 to 10000 cm<sup>2</sup>V<sup>-1</sup>s<sup>-1</sup> at room temperature. This means that good thermoelectric properties of nanoparticulate Bi<sub>2</sub>Te<sub>3</sub> near room temperature are also determined in part by the existence of surface charge carriers.