TY - JOUR
T1 - High-thermoelectric performance of nanostructured bismuth antimony telluride bulk alloys
AU - Poudel, Bed
AU - Hao, Qing
AU - Ma, Yi
AU - Lan, Yucheng
AU - Minnich, Austin
AU - Yu, Bo
AU - Yan, Xiao
AU - Wang, Dezhi
AU - Muto, Andrew
AU - Vashaee, Daryoosh
AU - Chen, Xiaoyuan
AU - Liu, Junming
AU - Dresselhaus, Mildred S.
AU - Chen, Gang
AU - Ren, Zhifeng
PY - 2008/5/2
Y1 - 2008/5/2
N2 - The dimensionless thermoelectric figure of merit (ZT) in bismuth antimony telluride (BiSbTe) bulk alloys has remained around 1 for more than 50 years. We show that a peak ZT of 1.4 at 100°C can be achieved in a p-type nanocrystalline BiSbTe bulk alloy. These nanocrystalline bulk materials were made by hot pressing nanopowders that were ball-milled from crystalline ingots under inert conditions. Electrical transport measurements, coupled with microstructure studies and modeling, show that the ZT improvement is the result of low thermal conductivity caused by the increased phonon scattering by grain boundaries and defects. More importantly, ZT is about 1.2 at room temperature and 0.8 at 250°C, which makes these materials useful for cooling and power generation. Cooling devices that use these materials have produced high-temperature differences of 86°, 106°, and 119°C with hot-side temperatures set at 50°, 100°, and 150°C, respectively. This discovery sets the stage for use of a new nanocomposite approach in developing high-performance low-cost bulk thermoelectric materials.
AB - The dimensionless thermoelectric figure of merit (ZT) in bismuth antimony telluride (BiSbTe) bulk alloys has remained around 1 for more than 50 years. We show that a peak ZT of 1.4 at 100°C can be achieved in a p-type nanocrystalline BiSbTe bulk alloy. These nanocrystalline bulk materials were made by hot pressing nanopowders that were ball-milled from crystalline ingots under inert conditions. Electrical transport measurements, coupled with microstructure studies and modeling, show that the ZT improvement is the result of low thermal conductivity caused by the increased phonon scattering by grain boundaries and defects. More importantly, ZT is about 1.2 at room temperature and 0.8 at 250°C, which makes these materials useful for cooling and power generation. Cooling devices that use these materials have produced high-temperature differences of 86°, 106°, and 119°C with hot-side temperatures set at 50°, 100°, and 150°C, respectively. This discovery sets the stage for use of a new nanocomposite approach in developing high-performance low-cost bulk thermoelectric materials.
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U2 - 10.1126/science.1156446
DO - 10.1126/science.1156446
M3 - Article
C2 - 18356488
AN - SCOPUS:46449085036
SN - 0036-8075
VL - 320
SP - 634
EP - 638
JO - Science
JF - Science
IS - 5876
ER -