TY - JOUR
T1 - Inhibiting the bipolar effect via band gap engineering to improve the thermoelectric performance in n-type Bi2-xSbxTe3 for solid-state refrigeration
AU - Su, Dongliang
AU - Cheng, Jiahui
AU - Li, Shan
AU - Zhang, Shengnan
AU - Lyu, Tu
AU - Zhang, Chaohua
AU - Li, Junqin
AU - Liu, Fusheng
AU - Hu, Lipeng
N1 - Publisher Copyright:
© 2022
PY - 2023/3/1
Y1 - 2023/3/1
N2 - To date, the benchmark Bi2Te3-based alloys are still the only commercial material system used for thermoelectric solid-state refrigeration. Nonetheless, the conspicuous performance imbalance between the p-type Bi2-xSbxTe3 and n-type Bi2Te3-xSex legs has become a major obstacle for the improvement of cooling devices to achieve higher efficiency. In our previous study, novel n-type Bi2-xSbxTe3 alloy has been proposed via manipulating donor-like effect as an alternative to mainstream n-type Bi2Te3-xSex. However, the narrow bandgap of Bi2-xSbxTe3 provoked severe bipolar effect that constrained the further improvement of zT near room temperature. Herein, we have implemented band gap engineering in n-type Bi1.5Sb0.5Te3 by employing isovalent Se substitution to inhibit the undesired intrinsic excitation and achieve the distinguished room-temperature zT. First, the preferential occupancy of Se at Te2 site appropriately enlarges the band gap, thereby concurrently improving the Seebeck coefficient and depressing the bipolar thermal conductivity. In addition, the Se alloying mildly suppresses the compensation mechanism and essentially preserves the already optimized carrier concentration, which maintains the peak zT near room temperature. Moreover, the large strain field and mass fluctuation generated by Se alloying leads to the remarkable reduction of lattice thermal conductivity. Accordingly, the zT value of Bi1.5Sb0.5Te2.8Se0.2 reaches 1.0 at 300 K and peaks 1.1 at 360 K, which surpasses that of most well-known room-temperature n-type thermoelectric materials. These results pave the way for n-type Bi2-xSbxTe3 alloys to become a new and promising top candidate for large-scale solid-state cooling applications.
AB - To date, the benchmark Bi2Te3-based alloys are still the only commercial material system used for thermoelectric solid-state refrigeration. Nonetheless, the conspicuous performance imbalance between the p-type Bi2-xSbxTe3 and n-type Bi2Te3-xSex legs has become a major obstacle for the improvement of cooling devices to achieve higher efficiency. In our previous study, novel n-type Bi2-xSbxTe3 alloy has been proposed via manipulating donor-like effect as an alternative to mainstream n-type Bi2Te3-xSex. However, the narrow bandgap of Bi2-xSbxTe3 provoked severe bipolar effect that constrained the further improvement of zT near room temperature. Herein, we have implemented band gap engineering in n-type Bi1.5Sb0.5Te3 by employing isovalent Se substitution to inhibit the undesired intrinsic excitation and achieve the distinguished room-temperature zT. First, the preferential occupancy of Se at Te2 site appropriately enlarges the band gap, thereby concurrently improving the Seebeck coefficient and depressing the bipolar thermal conductivity. In addition, the Se alloying mildly suppresses the compensation mechanism and essentially preserves the already optimized carrier concentration, which maintains the peak zT near room temperature. Moreover, the large strain field and mass fluctuation generated by Se alloying leads to the remarkable reduction of lattice thermal conductivity. Accordingly, the zT value of Bi1.5Sb0.5Te2.8Se0.2 reaches 1.0 at 300 K and peaks 1.1 at 360 K, which surpasses that of most well-known room-temperature n-type thermoelectric materials. These results pave the way for n-type Bi2-xSbxTe3 alloys to become a new and promising top candidate for large-scale solid-state cooling applications.
KW - Band gap
KW - BiTe
KW - Bipolar effect
KW - Point defects
KW - Thermoelectric
UR - http://www.scopus.com/inward/record.url?scp=85143822483&partnerID=8YFLogxK
U2 - 10.1016/j.jmst.2022.07.048
DO - 10.1016/j.jmst.2022.07.048
M3 - 文章
AN - SCOPUS:85143822483
SN - 1005-0302
VL - 138
SP - 50
EP - 58
JO - Journal of Materials Science and Technology
JF - Journal of Materials Science and Technology
ER -