铁电性
压电
材料科学
凝聚态物理
兴奋剂
结晶学
氮化物
纤锌矿晶体结构
压电系数
声子
电介质
纳米技术
化学
光电子学
物理
图层(电子)
复合材料
锌
冶金
作者
Jianan Sun,Jianfei Zhang,Junying Yan,Yinglong Wang,Jianzhong Lou,Xiaobing Yan,Jianxin Guo
标识
DOI:10.1002/pssb.202200079
摘要
Group III‐nitrides with doping recently attract great interest because of their outstanding ferroelectric and piezoelectric properties. Herein, the spontaneous polarization and piezoelectricity of the wurtzite III‐nitrides (AN, A = Al, Ga, In) with the rare earth element (R = Sc, Y) doping ( w ‐R 0.5 A 0.5 N) are investigated by first‐principles calculations. The polar w ‐R 0.5 A 0.5 N and nonpolar h ‐R 0.5 A 0.5 N are stable, which is proved by the elastic constants and phonon band structures. The w ‐Sc 0.5 In 0.5 N and w ‐Y 0.5 In 0.5 N can be applied to the ferroelectric field owing to their very small ferroelectric switching barriers (0.149 eV for w ‐Sc 0.5 In 0.5 N and 0.042 eV for w ‐Y 0.5 In 0.5 N) with large ferroelectric polarization (1.088 C m −2 for w ‐Sc 0.5 In 0.5 N and 0.937 C m −2 for w ‐Y 0.5 In 0.5 N). Furthermore, the w ‐Y 0.5 In 0.5 N has a large piezoelectric strain constant d 33 (14.018 pC N −1 ) based on the elastic constant C 33 softening and the increase of the piezoelectric constant e 33 , which is three times larger than that of w ‐InN (4.191 pC N −1 ). It is found that the biaxial tensile strain of 2% along in‐place significantly enhances the d 33 and e 33 , which increase to 35.572 pC N −1 and 2.669 C m −2 from 14.018 pC N −1 and 1.700 C m −2 of free w ‐Y 0.5 In 0.5 N, respectively.
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