Zhao Xiaodie, Ning Suiting, Qi Ning, Li Yuhuan, Dong Yun, Zhang Hongjun, Liu Jiandang, Ye Bangjiao, Chen Zhiquan
Hubei Nuclear Solid Physics Key Laboratory, Department of Physics, Wuhan University, Wuhan 430 072, China.
State Key Laboratory of Particle Detection and Electronics, University of Science and Technology of China, Hefei 230 026, China.
ACS Appl Mater Interfaces. 2021 Dec 15;13(49):58936-58948. doi: 10.1021/acsami.1c18818. Epub 2021 Dec 6.
In this study, a series of CuInSe (-0.3 ≤ ≤ 0.2 and 0 ≤ ≤ 0.05) samples were prepared by melting and the spark plasma sintering method. X-ray diffraction measurements indicate that the Cu-deficient samples ( = -0.3 = 0 and = -0.2 = 0) prefer to form the cubic phase (β-CuSe). Adding excessive Cu or introducing In atoms into the CuSe matrix triggers a phase transition from the β to α phase. Positron lifetime measurements confirm the reduction in Cu vacancy concentration by adding excessive Cu or introducing In atoms into CuSe, which causes a dramatic decrease in carrier concentration from 1.59 × 10 to 5.0 × 10 cm at room temperature. The samples with In contents of 0.01 and 0.03 show a high power factor of about 1 mW m K at room temperature due to the optimization of the carrier concentration. Meanwhile, the excess Cu content and doping of In atoms also favor the formation of nanopores. These pores have strong interaction with phonons, leading to remarkable reduction in lattice thermal conductivity. Finally, a high ZT value of about 1.44 is achieved at 873 K in the CuInSe ( = 0 and = 0.01) sample, which is about twice that of the Cu-deficient sample (CuSe). Our work provides a viable insight into tuning vacancy defects to improve efficiently the electrical and thermal transport performance for copper-based thermoelectric materials.
在本研究中,通过熔炼和放电等离子烧结法制备了一系列CuInSe(-0.3≤≤0.2且0≤≤0.05)样品。X射线衍射测量表明,缺铜样品(=-0.3 =0且=-0.2 =0)倾向于形成立方相(β-CuSe)。向CuSe基体中添加过量的Cu或引入In原子会引发从β相到α相的相变。正电子寿命测量证实,通过向CuSe中添加过量的Cu或引入In原子,Cu空位浓度降低,这导致室温下载流子浓度从1.59×10急剧降至5.0×10 cm。由于载流子浓度的优化,In含量为0.01和0.03的样品在室温下显示出约1 mW m K的高功率因子。同时,过量的Cu含量和In原子的掺杂也有利于纳米孔的形成。这些孔与声子有很强的相互作用,导致晶格热导率显著降低。最后,在873 K时,CuInSe(=0且=0.01)样品中实现了约1.44的高ZT值,约为缺铜样品(CuSe)的两倍。我们的工作为调整空位缺陷以有效改善铜基热电材料的电输运和热输运性能提供了可行的见解。