Akkopru-Akgun Betul, Trolier-McKinstry Susan
Center for Dielectrics and Piezoelectrics, Materials Research Institute, The Pennsylvania State University, University Park, PA 16802, USA.
Department of Materials Science and Engineering, The Pennsylvania State University, University Park, PA 16802, USA.
Materials (Basel). 2023 May 25;16(11):3970. doi: 10.3390/ma16113970.
Lead zirconate titanate (PZT) films with high Nb concentrations (6-13 mol%) were grown by chemical solution deposition. In concentrations up to 8 mol% Nb, the films self-compensate the stoichiometry; single phase films were grown from precursor solutions with 10 mol% PbO excess. Higher Nb concentrations induced multi-phase films unless the amount of excess PbO in the precursor solution was reduced. Phase pure perovskite films were grown with 13 mol% excess Nb with the addition of 6 mol% PbO. Charge compensation was achieved by creating lead vacancies when decreasing excess PbO level; using Kroger-Vink notation, NbTi• are ionically compensated by VPb″ to maintain charge neutrality in heavily Nb-doped PZT films. With Nb doping, films showed suppressed {100} orientation, the Curie temperature decreased, and the maximum in the relative permittivity at the phase transition broadened. The dielectric and piezoelectric properties were dramatically degraded due to increased quantity of the non-polar pyrochlore phase in multi-phase films; εr reduced from 1360 ± 8 to 940 ± 6, and the remanent d value decreased from 112 to 42 pm/V when increasing the Nb concentration from 6 to 13 mol%. Property deterioration was corrected by decreasing the PbO level to 6 mol%; phase pure perovskite films were attained. ε and the remanent d increased to 1330 ± 9 and 106 ± 4 pm/V, respectively. There was no discernable difference in the level of self-imprint in phase pure PZT films with Nb doping. However, the magnitude of the internal field after thermal poling at 150 °C increased significantly; the level of imprint was 30 kV/cm and 11.5 kV/cm in phase pure 6 mol% and 13 mol% Nb-doped films, respectively. The absence of mobile VO••, coupled with the immobile VPb″ in 13 mol% Nb-doped PZT films, leads to lower internal field formation upon thermal poling. For 6 mol% Nb-doped PZT films, the internal field formation was primarily governed by (1) the alignment of (VPb″-VO•• )x and (2) the injection and subsequent electron trapping by Ti. For 13 mol% Nb-doped PZT films, hole migration between VPb″ controlled internal field formation upon thermal poling.
通过化学溶液沉积法生长了具有高铌浓度(6 - 13摩尔%)的锆钛酸铅(PZT)薄膜。在铌浓度高达8摩尔%时,薄膜会自我补偿化学计量比;单相薄膜是由含10摩尔%过量氧化铅的前驱体溶液生长而成。更高的铌浓度会导致多相薄膜,除非前驱体溶液中过量氧化铅的量减少。通过添加6摩尔%的氧化铅,使用13摩尔%过量的铌生长出了相纯的钙钛矿薄膜。当降低过量氧化铅水平时,通过产生铅空位实现电荷补偿;使用克罗格 - 文克符号表示,在重铌掺杂的PZT薄膜中,NbTi•由VPb″进行离子补偿以保持电荷中性。随着铌掺杂,薄膜的{100}取向受到抑制,居里温度降低,相变时相对介电常数的最大值变宽。由于多相薄膜中非极性焦绿石相数量增加,介电和压电性能显著下降;当铌浓度从6摩尔%增加到13摩尔%时,εr从1360±8降至940±6,剩余d值从112降至42皮米/伏。通过将氧化铅水平降低到6摩尔%来纠正性能恶化;获得了相纯的钙钛矿薄膜。ε和剩余d分别增加到1330±9和106±4皮米/伏。在相纯的铌掺杂PZT薄膜中,自极化水平没有明显差异。然而,在150℃热极化后,内部电场强度显著增加;在相纯的6摩尔%和13摩尔%铌掺杂薄膜中,极化水平分别为30千伏/厘米和11.5千伏/厘米。在13摩尔%铌掺杂的PZT薄膜中,不存在可移动的VO••,且VPb″不可移动,这导致热极化时内部电场形成较低。对于6摩尔%铌掺杂的PZT薄膜,内部电场形成主要由(1)(VPb″ - VO•• )x的排列和(2)钛的注入及随后的电子俘获控制。对于13摩尔%铌掺杂的PZT薄膜,热极化时VPb″之间的空穴迁移控制内部电场形成。