High thermoelectric performance via hierarchical compositionally alloyed nanostructures.

Previous efforts to enhance thermoelectric performance have primarily focused on reduction in lattice thermal conductivity caused by broad-based phonon scattering across multiple length scales. Herein, we demonstrate a design strategy which provides for simultaneous improvement of electrical and thermal properties of p-type PbSe and leads to ZT ~ 1.6 at 923 K, the highest ever reported for a tellurium-free chalcogenide. Our strategy goes beyond the recent ideas of reducing thermal conductivity by adding two key new theory-guided concepts in engineering, both electronic structure and band alignment across nanostructure-matrix interface. Utilizing density functional theory for calculations of valence band energy levels of nanoscale precipitates of CdS, CdSe, ZnS, and ZnSe, we infer favorable valence band alignments between PbSe and compositionally alloyed nanostructures of CdS1-xSex/ZnS1-xSex. Then by alloying Cd on the cation sublattice of PbSe, we tailor the electronic structure of its two valence bands (light hole L and heavy hole Σ) to move closer in energy, thereby enabling the enhancement of the Seebeck coefficients and the power factor.

[1]  R. Opila,et al.  Preparation of clean Bi2Te3 and Sb2Te3 thin films to determine alignment at valence band maxima , 2011 .

[2]  D. Cahill,et al.  Lattice thermal conductivity of nanostructured thermoelectric materials based on PbTe , 2009 .

[3]  Weishu Liu,et al.  High-performance nanostructured thermoelectric materials , 2010 .

[4]  M. Kanatzidis Nanostructured Thermoelectrics: The New Paradigm?† , 2010 .

[5]  M. Kanatzidis,et al.  Cubic AgPbmSbTe2+m: Bulk Thermoelectric Materials with High Figure of Merit , 2004, Science.

[6]  M. Kanatzidis,et al.  High-performance bulk thermoelectrics with all-scale hierarchical architectures , 2012, Nature.

[7]  M. Dresselhaus,et al.  Recent developments in thermoelectric materials , 2003 .

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

[9]  Timothy P. Hogan,et al.  Raising the thermoelectric performance of p-type PbS with endotaxial nanostructuring and valence-band offset engineering using CdS and ZnS. , 2012, Journal of the American Chemical Society.

[10]  M. Kanatzidis,et al.  Thermoelectrics with earth abundant elements: high performance p-type PbS nanostructured with SrS and CaS. , 2012, Journal of the American Chemical Society.

[11]  Qian Zhang,et al.  Heavy doping and band engineering by potassium to improve the thermoelectric figure of merit in p-type PbTe, PbSe, and PbTe(1-y)Se(y). , 2012, Journal of the American Chemical Society.

[12]  Gang Chen,et al.  Recent advances in thermoelectric nanocomposites , 2012 .

[13]  M. Kanatzidis,et al.  High-performance tellurium-free thermoelectrics: all-scale hierarchical structuring of p-type PbSe-MSe systems (M = Ca, Sr, Ba). , 2013, Journal of the American Chemical Society.

[14]  M. Kanatzidis,et al.  New and old concepts in thermoelectric materials. , 2009, Angewandte Chemie.

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

[16]  Martin Hÿtch,et al.  Quantitative measurement of displacement and strain fields from HREM micrographs , 1998 .

[17]  G. T. Alekseeva Nature of hole localization centers in sodium-doped lead chalcogenides , 1997 .

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

[19]  M. Dresselhaus,et al.  Perspectives on thermoelectrics: from fundamentals to device applications , 2012 .

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

[21]  L. M. Rogers,et al.  Transport properties of the CdxPb1?x Te alloy system , 1971 .

[22]  M. Dresselhaus,et al.  High-Thermoelectric Performance of Nanostructured Bismuth Antimony Telluride Bulk Alloys , 2008, Science.

[23]  L. M. Rogers,et al.  Transport and optical properties of the CdxPb1-xSe and MgxPb1-xSe alloy systems , 1972 .

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

[25]  M. P. Walsh,et al.  Quantum Dot Superlattice Thermoelectric Materials and Devices , 2002, Science.

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

[27]  Heng Wang,et al.  Weak electron–phonon coupling contributing to high thermoelectric performance in n-type PbSe , 2012, Proceedings of the National Academy of Sciences.

[28]  M. Kanatzidis,et al.  High performance thermoelectrics from earth-abundant materials: enhanced figure of merit in PbS by second phase nanostructures. , 2011, Journal of the American Chemical Society.

[29]  G. J. Snyder,et al.  Combination of large nanostructures and complex band structure for high performance thermoelectric lead telluride , 2011 .

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

[31]  Joseph P. Heremans,et al.  Resonant levels in bulk thermoelectric semiconductors , 2012 .

[32]  Donald T. Morelli,et al.  Thermopower enhancement in lead telluride nanostructures , 2004 .

[33]  Ali Shakouri,et al.  Nanostructured Thermoelectrics: Big Efficiency Gains from Small Features , 2010, Advanced materials.

[34]  M. Kanatzidis Chapter 3 The role of solid-state chemistry in the discovery of new thermoelectric materials , 2001 .

[35]  G. J. Snyder,et al.  Complex thermoelectric materials. , 2008, Nature materials.