No‐Heating Deposition of Ferroelectric x%YO1.5–(100−x%)(Hf1−yZry)O2 Films

T. Mimura, Reijiro Shimura, Akinori Tateyama, Y. Nakamura, T. Shiraishi, H. Funakubo
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Abstract

The no‐heating deposition of x%YO1.5–(100−x%)(Hf1−yZry)O2 (x = 0−0.09, y = 0, 0.25, 0.50, and 1) is achieved using a radio‐frequency magnetron sputtering method. To investigate the crystal structure and ferroelectric properties, epitaxial films are grown on (111)‐oriented indium tin oxide (ITO)/(111) Y‐stabilized zirconia (YSZ) substrates. The ferroelectric orthorhombic phase is obtained for the 5–7%YO1.5–95–93%HfO2 and 5%YO1.5–95% (Hf0.75Zr0.25)O2 films. The field‐induced phase transition from tetragonal to orthorhombic is confirmed for the 8%YO1.5–92%HfO2 and 5%YO1.5–95%(Hf0.50Zr0.50)O2 films. The remnant polarization (Pr) and coercive field (Ec) are 12–19 μC cm−2 and 2,000–2,500 kV cm−1, respectively. The piezoelectric response of 1 μm thick films is investigated for 6%YO1.5–94% HfO2, 7%YO1.5–93%HfO2, and 5%YO1.5–95%(Hf0.50Zr0.50)O2 films, which have piezoelectric coefficients (d33) of 1.0, 3.3, and 5.0 pm V−1, respectively. These results show no‐heating deposition of x%YO1.5–(100−x%)(Hf1−yZry)O2 films with ferroelectric and piezoelectric properties.
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铁电x%YO1.5 -(100−x%)(Hf1−yZry)O2薄膜的无加热沉积
采用射频磁控溅射方法,实现了x%YO1.5 -(100−x%)(Hf1−yZry)O2 (x = 0−0.09,y = 0, 0.25, 0.50和1)的无加热沉积。为了研究晶体结构和铁电性能,在(111)取向氧化铟锡(ITO)/(111) Y稳定氧化锆(YSZ)衬底上生长外延薄膜。在5-7%YO1.5-95-93%HfO2和5%YO1.5-95% (Hf0.75Zr0.25)O2薄膜中获得了铁电正交相。在8%YO1.5-92%HfO2和5%YO1.5-95% (Hf0.50Zr0.50)O2薄膜中,证实了场致相变从四方向正交相转变。残余极化(Pr)和矫顽力场(Ec)分别为12 ~ 19 μC cm−2和2000 ~ 2500 kV cm−1。研究了6% yo1.5 ~ 94% HfO2、7% yo1.5 ~ 93%HfO2和5% yo1.5 ~ 95%(Hf0.50Zr0.50)O2薄膜对1 μm厚薄膜的压电响应,这些薄膜的压电系数(d33)分别为1.0、3.3和5.0 pm V−1。这些结果表明,无加热沉积的x%YO1.5 -(100−x%)(Hf1−yZry)O2薄膜具有铁电和压电性能。
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