TY - JOUR
T1 - Valence-band structure of highly efficient p-type thermoelectric PbTe-PbS alloys
AU - Jaworski, Christopher M.
AU - Nielsen, Michele D.
AU - Wang, Hsin
AU - Girard, Steven N.
AU - Cai, Wei
AU - Porter, Wally D.
AU - Kanatzidis, Mercouri G.
AU - Heremans, Joseph P.
PY - 2013/1/4
Y1 - 2013/1/4
N2 - Experimental evidence is given relevant to the temperature dependence of the valence band structure of PbTe and PbTe1-xSxaloys (0.04≤x≤0.12), and its effect on the thermoelectric figure of merit ZT. The x=0.08 sample has ZT∼1.55 at 773 K. The magnetic field dependence of the high-temperature Hall resistivity of heavily p-type (>1019 cm-3) Na-doped PbTe1-xSx reveals the presence of high-mobility electrons. This casts doubts on prior analyses of the Hall coefficient suggesting that temperature induces a rapid rise in energy of the "heavy" hole relative to the "light" hole bands. The electron-like behavior is likely induced by the topology of the Fermi surface when the L- and Σ-bands merge. Negative values for the low-temperature thermopower are also observed. The data show that PbTe continues to be a direct-gap semiconductor at temperatures where the ZT and S2σ of p-type PbTe are optimal, e.g., 700-800 K.
AB - Experimental evidence is given relevant to the temperature dependence of the valence band structure of PbTe and PbTe1-xSxaloys (0.04≤x≤0.12), and its effect on the thermoelectric figure of merit ZT. The x=0.08 sample has ZT∼1.55 at 773 K. The magnetic field dependence of the high-temperature Hall resistivity of heavily p-type (>1019 cm-3) Na-doped PbTe1-xSx reveals the presence of high-mobility electrons. This casts doubts on prior analyses of the Hall coefficient suggesting that temperature induces a rapid rise in energy of the "heavy" hole relative to the "light" hole bands. The electron-like behavior is likely induced by the topology of the Fermi surface when the L- and Σ-bands merge. Negative values for the low-temperature thermopower are also observed. The data show that PbTe continues to be a direct-gap semiconductor at temperatures where the ZT and S2σ of p-type PbTe are optimal, e.g., 700-800 K.
UR - http://www.scopus.com/inward/record.url?scp=84872253340&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.87.045203
DO - 10.1103/PhysRevB.87.045203
M3 - Article
AN - SCOPUS:84872253340
SN - 1098-0121
VL - 87
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 4
M1 - 045203
ER -