Abstract
The study presented here includes experimental data obtained from three n-type and two p-type single-crystalline samples of PbTe. Measurements of the Hall coefficient, thermoelectric power, and electrical conductivity have been made between 77 and 300°K, and infrared reflectivity data have been obtained at 4, 77, 190, and 300°K. The free-carrier concentration of all samples is in the range 2-4×1018 carriers/cm3. From the thermoelectric power, we have deduced the temperature dependence of the reduced Fermi potential for each sample and have calculated the density-of-states effective mass md. A pronounced temperature dependence has been observed for md. At 77°K we have observed that mdn=0.20 mo and mdp=0.14 mo, whereas at 300°K they have increased monotonically to the values mdn=0.30 mo and mdp=0.25 mo. The minimum of the infrared reflectivity has been utilized in obtaining values for the conductivity effective mass mc. The temperature dependence noted for mc has been very similar to that obtained for md. At 4°K we obtained the values mcn=0.050 mo and mcp=0.039 mo, and they increase monotonically to their values at 300°K which have been determined to be mcn=0.103 mo and mcp=0.11 mo. These values of the effective masses have been used to deduce the number of equivalent ellipsoids of constant energy Nv. For the conduction band, we find Nv=4 indicating that the (111) minima are at the edge of the zone. For the valence band we are unable to be as quantitative because of the presence of a maximum at the center of the zone as well as the maxima positioned along the 111 axes. However, assuming that all ellipsoids are equivalent, we calculate Nv2.5 from which it is inferred that the zone-centered maximum plays a prominent role in the energy-band picture.