Superparamagnetic enhancement of thermoelectric performance

The ability to control chemical and physical structuring at the nanometre scale is important for developing high-performance thermoelectric materials. Progress in this area has been achieved mainly by enhancing phonon scattering and consequently decreasing the thermal conductivity of the lattice through the design of either interface structures at nanometre or mesoscopic length scales or multiscale hierarchical architectures. A nanostructuring approach that enables electron transport as well as phonon transport to be manipulated could potentially lead to further enhancements in thermoelectric performance. Here we show that by embedding nanoparticles of a soft magnetic material in a thermoelectric matrix we achieve dual control of phonon- and electron-transport properties. The properties of the nanoparticles—in particular, their superparamagnetic behaviour (in which the nanoparticles can be magnetized similarly to a paramagnet under an external magnetic field)—lead to three kinds of thermoelectromagnetic effect: charge transfer from the magnetic inclusions to the matrix; multiple scattering of electrons by superparamagnetic fluctuations; and enhanced phonon scattering as a result of both the magnetic fluctuations and the nanostructures themselves. We show that together these effects can effectively manipulate electron and phonon transport at nanometre and mesoscopic length scales and thereby improve the thermoelectric performance of the resulting nanocomposites.

[1]  E. Wohlfarth,et al.  The Curie temperature of the ferromagnetic transition metals and their compounds , 1987 .

[2]  B. Diény,et al.  Estimation of the Co nanoparticles size by magnetic measurements in Co/SiO2 discontinuous multilayers , 2004 .

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

[4]  Tiejun Zhu,et al.  Realizing high figure of merit in heavy-band p-type half-Heusler thermoelectric materials , 2015, Nature communications.

[5]  H. Michaelson The work function of the elements and its periodicity , 1977 .

[6]  Q. Jiang,et al.  Size and interface effects on critical temperatures of ferromagnetic, ferroelectric and superconductive nanocrystals , 2005 .

[7]  P. Zhai,et al.  Synthesis and high temperature transport properties of barium and indium double-filled skutterudites BaxInyCo4Sb12−z , 2007 .

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

[9]  T. Okamoto,et al.  Temperature Dependence of the Magnetocrystalline Anisotropy Constants K1 and K2 of Nickel , 1965 .

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

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

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

[13]  Yongli Gao,et al.  Surface analytical studies of interfaces in organic semiconductor devices , 2010 .

[14]  Chunlei Dong,et al.  Enhanced thermoelectric performance in barium and indium double-filled skutterudite bulk materials via orbital hybridization induced by indium filler. , 2009, Journal of the American Chemical Society.

[15]  R. L. Fitzpatrick,et al.  Electronic Transport in Semimetallic Cerium Sulfide , 1964 .

[16]  Jihui Yang,et al.  Multi-localization transport behaviour in bulk thermoelectric materials , 2015, Nature Communications.

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

[18]  M. Dresselhaus,et al.  New Directions for Low‐Dimensional Thermoelectric Materials , 2007 .

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

[20]  R. Bozorth Directional Ferromagnetic Properties of Metals , 1937 .

[21]  Xianli Su,et al.  Magnetoelectric interaction and transport behaviours in magnetic nanocomposite thermoelectric materials. , 2017, Nature nanotechnology.

[22]  Jian Yu,et al.  Enhanced thermoelectric performance via randomly arranged nanopores: Excellent transport properties of YbZn2Sb2 nanoporous materials , 2012 .

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

[24]  G. J. Snyder,et al.  Copper ion liquid-like thermoelectrics. , 2012, Nature materials.

[25]  Min Zhou,et al.  Nanostructured AgPb(m)SbTe(m+2) system bulk materials with enhanced thermoelectric performance. , 2008, Journal of the American Chemical Society.

[26]  R. K. Williams,et al.  Filled Skutterudite Antimonides: A New Class of Thermoelectric Materials , 1996, Science.

[27]  C. Uher,et al.  Anomalous barium filling fraction and n-type thermoelectric performance of BayCo4Sb12 , 2001 .

[28]  P. T. Pappas,et al.  The original Ampère force and Biot-Savart and Lorentz forces , 1983 .

[29]  Victor I. Fistul,et al.  Preparation of Heavily Doped Semiconductors , 1969 .

[30]  H. Takizawa,et al.  Polarized Raman-scattering study of Ge and Sn-filled CoSb3 , 2003 .

[31]  M. Kanatzidis,et al.  Broad temperature plateau for thermoelectric figure of merit ZT>2 in phase-separated PbTe0.7S0.3 , 2014, Nature Communications.

[32]  J. Thompson,et al.  The magnetic anisotropy of cobalt , 1954, Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences.

[33]  Q. Jiang,et al.  Glass transition of low-dimensional polystyrene , 2004 .

[34]  M. Dresselhaus,et al.  Spectral mapping of thermal conductivity through nanoscale ballistic transport. , 2015, Nature nanotechnology.

[35]  Wei Liu,et al.  Convergence of conduction bands as a means of enhancing thermoelectric performance of n-type Mg2Si(1-x)Sn(x) solid solutions. , 2012, Physical review letters.

[36]  Zhiwei Zhou,et al.  Progressive Regulation of Electrical and Thermal Transport Properties to High‐Performance CuInTe2 Thermoelectric Materials , 2016 .

[37]  D. Wood Classical size dependence of the work function of small metallic spheres , 1981 .

[38]  G. J. Snyder,et al.  Disordered zinc in Zn4Sb3 with phonon-glass and electron-crystal thermoelectric properties , 2004, Nature materials.

[39]  David W. McComb,et al.  Observation of spin Seebeck contribution to the transverse thermopower in Ni-Pt and MnBi-Au bulk nanocomposites , 2016, Nature communications.