High Thermoelectric Power Factor of High‐Mobility 2D Electron Gas

Abstract Thermoelectric conversion is an energy harvesting technology that directly converts waste heat from various sources into electricity by the Seebeck effect of thermoelectric materials with a large thermopower (S), high electrical conductivity (σ), and low thermal conductivity (κ). State‐of‐the‐art nanostructuring techniques that significantly reduce κ have realized high‐performance thermoelectric materials with a figure of merit (ZT = S 2∙σ∙T∙κ−1) between 1.5 and 2. Although the power factor (PF = S 2∙σ) must also be enhanced to further improve ZT, the maximum PF remains near 1.5–4 mW m−1 K−2 due to the well‐known trade‐off relationship between S and σ. At a maximized PF, σ is much lower than the ideal value since impurity doping suppresses the carrier mobility. A metal‐oxide‐semiconductor high electron mobility transistor (MOS‐HEMT) structure on an AlGaN/GaN heterostructure is prepared. Applying a gate electric field to the MOS‐HEMT simultaneously modulates S and σ of the high‐mobility electron gas from −490 µV K−1 and ≈10−1 S cm−1 to −90 µV K−1 and ≈104 S cm−1, while maintaining a high carrier mobility (≈1500 cm2 V−1 s−1). The maximized PF of the high‐mobility electron gas is ≈9 mW m−1 K−2, which is a two‐ to sixfold increase compared to state‐of‐the‐art practical thermoelectric materials.

[1]  Tamotsu Hashizume,et al.  Characterization of interface states in Al2O3/AlGaN/GaN structures for improved performance of high-electron-mobility transistors , 2013 .

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

[3]  Cronin B. Vining,et al.  A model for the high‐temperature transport properties of heavily doped n‐type silicon‐germanium alloys , 1991 .

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

[5]  D. M. Rowe,et al.  Phonon scattering at grain boundaries in heavily doped fine-grained silicon–germanium alloys , 1981, Nature.

[6]  K. Nakahara,et al.  Thermoelectric enhancement in the two‐dimensional electron gas of AlGaN/GaN heterostructures , 2016 .

[7]  Tamotsu Hashizume,et al.  Highly-stable and low-state-density Al2O3/GaN interfaces using epitaxial n-GaN layers grown on free-standing GaN substrates , 2016 .

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

[9]  H. Ohta,et al.  Unusually Large Enhancement of Thermopower in an Electric Field Induced Two‐Dimensional Electron Gas , 2011, Advanced materials.

[10]  H. Ohta,et al.  Field-modulated thermopower in SrTiO3-based field-effect transistors with amorphous 12CaO⋅7Al2O3 glass gate insulator , 2009 .

[11]  Hideo Hosono,et al.  Giant thermoelectric Seebeck coefficient of a two-dimensional electron gas in SrTiO3. , 2007, Nature materials.

[12]  C. B. Vining An inconvenient truth about thermoelectrics. , 2009, Nature materials.

[13]  R. Cava,et al.  Large enhancement of the thermopower in NaxCoO2 at high Na doping , 2006, Nature materials.

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

[15]  H. Angerer,et al.  Thermopower investigation of n- and p-type GaN , 1998 .

[16]  Terry M. Tritt,et al.  Thermoelectric Materials, Phenomena, and Applications: A Bird’s Eye View , 2006 .

[17]  M. Dresselhaus,et al.  Quantum Effects in the Thermoelectric Power Factor of Low-Dimensional Semiconductors. , 2016, Physical review letters.

[18]  T. Hashizume,et al.  Process Conditions for Improvement of Electrical Properties of Al2O3/n-GaN Structures Prepared by Atomic Layer Deposition , 2010 .

[19]  K. Pernstich,et al.  Field-effect-modulated Seebeck coefficient in organic semiconductors. , 2008, Nature materials.

[20]  S. Denbaars,et al.  High temperature thermoelectric properties of optimized InGaN , 2011 .

[21]  A. Majumdar,et al.  Enhanced thermoelectric performance of rough silicon nanowires , 2008, Nature.

[22]  Xin Li,et al.  Alloy‐scattering dependence of electron mobility in the ternary gallium, indium, and aluminum nitrides , 1995 .

[23]  Tanakorn Osotchan,et al.  Electron mobilities in gallium, indium, and aluminum nitrides , 1994 .

[24]  Uher,et al.  CsBi(4)Te(6): A high-performance thermoelectric material for low-temperature applications , 2000, Science.

[25]  G. J. Snyder,et al.  Dense dislocation arrays embedded in grain boundaries for high-performance bulk thermoelectrics , 2015, Science.

[26]  Heng Wang,et al.  Ultrahigh power factor and thermoelectric performance in hole-doped single-crystal SnSe , 2016, Science.

[27]  Tamotsu Hashizume,et al.  Insulated gate and surface passivation structures for GaN-based power transistors , 2016 .

[28]  Mildred S. Dresselhaus,et al.  Effect of quantum-well structures on the thermoelectric figure of merit. , 1993, Physical review. B, Condensed matter.

[29]  P. Han,et al.  Study of two‐dimensional electron gas in AlN/GaN heterostructure by a self‐consistent method , 2004 .

[30]  Yuan Liu,et al.  Achieving high power factor and output power density in p-type half-Heuslers Nb1-xTixFeSb , 2016, Proceedings of the National Academy of Sciences.

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

[32]  H. Ohta,et al.  Field-induced water electrolysis switches an oxide semiconductor from an insulator to a metal , 2010, Nature communications.