Ziye Zhu1,2,3,Xiaoping Yao1,2,3,Shu Zhao1,2,3,Xiao Lin1,2,Wenbin Li1,2
Westlake University1,Westlake Institute for Advanced Study2,Zhejiang University3
Ziye Zhu1,2,3,Xiaoping Yao1,2,3,Shu Zhao1,2,3,Xiao Lin1,2,Wenbin Li1,2
Westlake University1,Westlake Institute for Advanced Study2,Zhejiang University3
We find that the ultrahigh electron mobility observed in the layered semiconductor Bi<sub>2</sub>O<sub>2</sub>Se originates from an incipient ferroelectric transition that endows the material a large dielectric permittivity, providing it with a robust protection against mobility degradation by Coulomb scattering. Based on state-of-the-art first-principles calculations, we show that the low-temperature electron mobility of Bi<sub>2</sub>O<sub>2</sub>Se, taking into account both electron-phonon and ionized impurity scattering, can reach 10<sup>4 </sup>to 10<sup>7 </sup>cm<sup>2</sup>V<sup>−1</sup>s<sup>−1 </sup>over a wide range of realistic doping levels. Moreover, a small elastic strain of 1.7% can drive Bi<sub>2</sub>O<sub>2</sub>Se toward the ferroelectric phase transition, inducing a giant increase in the permittivity and enables the strain-tuning of low-temperature electron mobility by more than an order of magnitude. These results establish a new route for realizing high-mobility<br/>layered semiconductors via phase and dielectric engineering.