Exploring the doping effects of Ag in p-type PbSe compounds with enhanced thermoelectric performance

In this study, we prepared a series of Ag-doped PbSe bulk materials by a melting–quenching process combined with a subsequent spark plasma sintering process, and systematically investigated the doping effects of Ag on the thermoelectric properties. Ag substitution in the Pb site does not introduce resonant levels near the valence band edge or detectable change in the density of state in the vicinity of the Fermi level, but moves the Fermi level down and increases the carrier concentration to a maximum value of ∼4.7 × 1019 cm−3 which is still insufficient for heavily doped PbSe compounds. Nonetheless, the non-monotonic variation in carrier concentration with increasing Ag content indicates that Ag doping reaches the solution limit at ∼1.0% and the excessive Ag presumably acts as donors in the materials. Moreover, the large energy gap of the PbSe-based material wipes off significant ‘roll-over’ in the Seebeck coefficient at elevated temperatures which gives rise to high power factors, being comparable to p-type Te analogues. Consequently, the maximum ZT reaches ∼1.0 for the 1.5% Ag-doped samples with optimized carrier density, which is ∼70% improvement in comparison with an undoped sample and also superior to the commercialized p-type PbTe materials.

[1]  Yue Wu,et al.  Nanostructure-based thermoelectric conversion: an insight into the feasibility and sustainability for large-scale deployment. , 2011, Nanoscale.

[2]  Shanyu Wang,et al.  Enhanced performances of melt spun Bi2(Te,Se)3 for n-type thermoelectric legs , 2011 .

[3]  M. Kanatzidis,et al.  Thermoelectrics from abundant chemical elements: high-performance nanostructured PbSe-PbS. , 2011, Journal of the American Chemical Society.

[4]  G. J. Snyder,et al.  High thermoelectric figure of merit in heavy hole dominated PbTe , 2011 .

[5]  M. Kanatzidis,et al.  High-temperature thermoelectric properties of n-type PbSe doped with Ga, In, and Pb , 2011 .

[6]  Heng Wang,et al.  Convergence of electronic bands for high performance bulk thermoelectrics , 2011, Nature.

[7]  G. J. Snyder,et al.  Self‐Tuning the Carrier Concentration of PbTe/Ag2Te Composites with Excess Ag for High Thermoelectric Performance , 2011 .

[8]  G. J. Snyder,et al.  Heavily Doped p‐Type PbSe with High Thermoelectric Performance: An Alternative for PbTe , 2011, Advanced materials.

[9]  M. Kanatzidis,et al.  Nanostructures boost the thermoelectric performance of PbS. , 2011, Journal of the American Chemical Society.

[10]  M. Kanatzidis,et al.  Strained endotaxial nanostructures with high thermoelectric figure of merit. , 2011, Nature chemistry.

[11]  Anthony V. Powell,et al.  Recent developments in nanostructured materials for high-performance thermoelectrics , 2010 .

[12]  Shanyu Wang,et al.  High performance n-type (Bi,Sb)2(Te,Se)3 for low temperature thermoelectric generator , 2010 .

[13]  M. Kanatzidis,et al.  Thermoelectric enhancement in PbTe with K or Na codoping from tuning the interaction of the light- and heavy-hole valence bands , 2010, 1007.1637.

[14]  David J. Singh,et al.  High-temperature thermoelectric performance of heavily doped PbSe , 2010 .

[15]  M. Kanatzidis,et al.  Improvement in the Thermoelectric Figure of Merit by La/Ag Cosubstitution in PbTe , 2009 .

[16]  Ctirad Uher,et al.  Large enhancements in the thermoelectric power factor of bulk PbTe at high temperature by synergistic nanostructuring. , 2008, Angewandte Chemie.

[17]  L. Bell Cooling, Heating, Generating Power, and Recovering Waste Heat with Thermoelectric Systems , 2008, Science.

[18]  G. J. Snyder,et al.  Enhancement of Thermoelectric Efficiency in PbTe by Distortion of the Electronic Density of States , 2008, Science.

[19]  M. P. Walsh,et al.  Carrier concentration and temperature dependence of the electronic transport properties of epitaxial PbTe and PbTe/PbSe nanodot superlattices , 2008 .

[20]  Lidong Chen,et al.  Thermoelectrics: Direct Solar Thermal Energy Conversion , 2008 .

[21]  G. J. Snyder,et al.  Effect of disorder on the thermal transport and elastic properties in thermoelectric Zn 4 Sb 3 , 2006 .

[22]  Chang Q. Sun,et al.  Size-induced acoustic hardening and optic softening of phonons in InP, CeO2, SnO2, CdS, Ag, and Si nanostructures , 2005 .

[23]  H. Goldsmid,et al.  Estimation of the thermal band gap of a semiconductor from seebeck measurements , 1999 .

[24]  Terry M. Tritt,et al.  Holey and Unholey Semiconductors , 1999, Science.

[25]  Zettl,et al.  Variable Hall coefficient in Bi2Sr2CaCu2O8-x across the metal-insulator transition. , 1989, Physical review. B, Condensed matter.

[26]  L. M. Rogers,et al.  Interpretation of the Hall coefficient, electrical resistivity and Seebeck coefficient of p-type lead telluride , 1967 .

[27]  George S. Nolas,et al.  Thermoelectrics: Basic Principles and New Materials Developments , 2001 .

[28]  L. Stil’bans,et al.  Semiconducting Lead Chalcogenides , 1970 .

[29]  L. Stil’bans,et al.  Physical problems of thermoelectricity , 1959 .