材料科学
铁电性
正交晶系
四方晶系
凝聚态物理
空位缺陷
偶极子
化学计量学
极化(电化学)
结晶学
分析化学(期刊)
电介质
光电子学
晶体结构
物理化学
化学
物理
有机化学
色谱法
作者
Jinchen Wei,Lilai Jiang,Menglin Huang,Yu‐Ning Wu,Shiyou Chen
标识
DOI:10.1002/adfm.202104913
摘要
Abstract It is believed that promoting the fraction of ferroelectric orthorhombic phase (o‐phase) through O‐poor growth conditions can increase the spontaneous polarization of HfO 2 and (Hf,Zr)O 2 thin films. However, the first‐principles calculations show that the growth may be limited by the easy formation of point defects in the orthorhombic and tetragonal phases of HfO 2 , ZrO 2 , and (Hf,Zr)O 2 . Their dominant defects, O interstitial (O i ) under O‐rich conditions and O vacancy ( V O ) under O‐poor condition, have low formation energies and quite high density (10 16 –10 19 cm −3 for 800–1400 K growth temperature). Especially, O i has negative formation energy in tetragonal HfO 2 under O‐rich condition, causing non‐stoichiometry and limiting the crystalline‐seed formation during o‐phase growth. High‐density defects can cause disordering of dipole moments and increase leakage current, both diminishing the polarization. These results explain the experimental puzzle that the measured polarization is much lower than the ideal value even in O‐poor thin films and highlight that controlling defects is as important as promoting the o‐phase fraction for enhancing ferroelectricity. The O‐intermediate condition (average of O‐rich and O‐poor conditions) and low growth temperature are proposed for fabricating HfO 2 and (Hf,Zr)O 2 with fewer defects, lower leakage current, and stronger ferroelectricity, which challenges the belief that O‐poor condition is optimal.
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