Yu Xiao

Yu Xiao


Research Focus & Metrics

Academic Career Length

10Years (2017-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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27 September 2019 in Science
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Journal Article
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WHWenke He
Wenke He
DWDongyang Wang
Dongyang Wang
Haijun WuHaijun Wu
Haijun Wu
YXYu Xiao
Yu Xiao
YZYang Zhang
Yang Zhang
Li-Dong ZhaoLi-Dong Zhao
Li-Dong Zhao
Lower-cost thermoelectrics: Thermoelectric materials convert heat to electricity, making them attractive for heat harvesting or cooling applications. However, many high-performance thermoelectrics are made of expensive or toxic materials. He et al. found that a material composed of primarily tin and sulfur could be optimized to have relatively good thermoelectric properties. Introducing about 10% selenium to tin sulfide helped tune these properties by electronic band manipulation. This material is a step toward more earth-abundant, less toxic, and lower-cost thermoelectrics than the telluride-based materials currently in use. Science , this issue p. 1418

4 February 2020 in Journal of the American Chemical Society
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Journal Article
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YXYu Xiao
Yu Xiao
DWDongyang Wang
Dongyang Wang
YZYang Zhang
Yang Zhang
CCCongrun Chen
Congrun Chen
SZShuxuan Zhang
Shuxuan Zhang
Li-Dong ZhaoLi-Dong Zhao
Li-Dong Zhao

28 October 2022 in Nature Communications
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LXLiqing Xu
Liqing Xu
YXYu Xiao
Yu Xiao
SWSining Wang
Sining Wang
BCBo Cui
Bo Cui
DWDi Wu
Di Wu
Li-Dong ZhaoLi-Dong Zhao
Li-Dong Zhao
PbSe-based thermoelectric materials exhibit promising ZT values at medium temperature, but its near-room-temperature thermoelectric properties are overlooked, thus restricting its average ZT (ZTave) value at low-medium temperatures. Here, a high ZTave of 0.90 at low temperature (300–573 K) is reported in n-type PbSe-based thermoelectric material (Pb1.02Se0.72Te0.20S0.08−0.3%Cu), resulting in a large ZTave of 0.96 at low-medium temperatures (300–773 K). This high thermoelectric performance stems from its ultralow lattice thermal conductivity caused by dense dislocations through heavy Te/S alloying and Cu interstitial doping. The dislocation density evaluated by modified Williamson-Hall method reaches up to 5.4 × 1016 m−2 in Pb1.02Se0.72Te0.20S0.08−0.3%Cu. Moreover, the microstructure observation further uncloses two kinds of dislocations, namely screw and edge dislocations, with several to hundreds of nanometers scale in length. These dislocations in lattice can strongly intensify phonon scattering to minimize the lattice thermal conductivity and simultaneously maintain high carrier transport. As a result, with the reduced lattice thermal conductivity and optimized power factor in Pb1.02Se0.72Te0.20S0.08−0.3%Cu, its near-room-temperature thermoelectric performance is largely enhanced and exceeds previous PbSe-based thermoelectric materials.

8 August 2022 in Interdisciplinary Materials
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Open access
ZLZhengtao Liu
Zhengtao Liu
THTao Hong
Tao Hong
LXLiqing Xu
Liqing Xu
SWSining Wang
Sining Wang
XGXiang Gao
Xiang Gao
Li-Dong ZhaoLi-Dong Zhao
Li-Dong Zhao
Lead sulfide (PbS) presents large potential in thermoelectric application due to its earth‐abundant S element. However, its inferior average ZT (ZTave) value makes PbS less competitive with its analogs PbTe and PbSe. To promote its thermoelectric performance, this study implements strategies of continuous Se alloying and Cu interstitial doping to synergistically tune thermal and electrical transport properties in n‐type PbS. First, the lattice parameter of 5.93 Å in PbS is linearly expanded to 6.03 Å in PbS0.5Se0.5 with increasing Se alloying content. This expanded lattice in Se‐alloyed PbS not only intensifies phonon scattering but also facilitates the formation of Cu interstitials. Based on the PbS0.6Se0.4 content with the minimal lattice thermal conductivity, Cu interstitials are introduced to improve the electron density, thus boosting the peak power factor, from 3.88 μW cm−1 K−2 in PbS0.6Se0.4 to 20.58 μW cm−1 K−2 in PbS0.6Se0.4−1%Cu. Meanwhile, the lattice thermal conductivity in PbS0.6Se0.4−x%Cu (x = 0–2) is further suppressed due to the strong strain field caused by Cu interstitials. Finally, with the lowered thermal conductivity and high electrical transport properties, a peak ZT ~1.1 and ZTave ~0.82 can be achieved in PbS0.6Se0.4 − 1%Cu at 300–773K, which outperforms previously reported n‐type PbS.

25 November 2021 in Energy & Environmental Science
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YXYu Xiao
Yu Xiao
LXLiqing Xu
Liqing Xu
THTao Hong
Tao Hong
HSHaonan Shi
Haonan Shi
SWSining Wang
Sining Wang
Li-Dong ZhaoLi-Dong Zhao
Li-Dong Zhao
Carrier mobility is a key parameter for thermoelectric performance. A high average ZT value of ∼1.13 can be achieved in n-type PbSe–18%SnS–0.5%Cu at 300–873 K through the rational optimization of carrier mobility.

13 March 2022 in Advanced Energy Materials
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Journal Article
Closed access
YXYu Xiao
Yu Xiao
HWHaijun Wu
Haijun Wu
HSHaonan Shi
Haonan Shi
LXLiqing Xu
Liqing Xu
YZYuke Zhu
Yuke Zhu
Li-Dong ZhaoLi-Dong Zhao
Li-Dong Zhao