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High retention of the polarization and depolarization field in polycrystalline metal/Pb(ZrTi)O_3/metal capacitors

机译:多晶金属/ Pb(ZrTi)O_3 /金属电容器中极化和去极化场的高度保留

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摘要

Long term relaxation of the photovoltaic current in poled and then short-circuited capacitors with polycrystalline Pb(ZrTi)O_3 (PZT) film, where (111) oriented PZT grains are separated by ultrathin semiconductor PbO phase is studied. The quantum energy of the excitation light is lower than PZT band gap but higher than PbO band gap. The measured photovoltaic current differs entirely from well-known photovoltaic current observed in single-crystal ferroelectrics, which flows in polarization direction and originates due to asymmetry of impurity potential caused by the polarization. The photocurrent, which we measure, is always directed against the polarization and is not related to the depolarization of the film. The driving force of the measured photocurrent is the depolarization field generated by polarization charge on PZT grain boundaries [Delimova et al., Appl. Phys. Lett. 91, 112907 (2007)]. Photoexcited in PbO interlayers free carriers drift in this field toward electrodes producing the photocurrent, which can serve as a criterion of existence of the depolarization field. It is shown that the steady-state photovoltaic current in poled M/PZT/M capacitors, measured for a year without their repolarization, demonstrates only 30% decrease. This means that during the year the depolarization field has remained in the film, the polarization charge generating the depolarization field has not been compensated, thereby indicating that the polarization is also conserved. The calculation of the photocurrent, depolarization field and polarization, performed using two-dimensional phenomenological model, shows that the polarization charge on grain boundaries cannot be compensated completely neither by free carriers nor charged dopants, which confirms the experimental result.
机译:研究了具有多晶Pb(ZrTi)O_3(PZT)膜的极化和短路电容器中光伏电流的长期松弛,其中(111)取向的PZT晶粒被超薄半导体PbO相隔开。激发光的量子能低于PZT带隙但高于PbO带隙。测得的光伏电流与在单晶铁电体中观察到的众所周知的光伏电流完全不同,后者在偏振方向上流动,并且是由于偏振引起的杂质电势的不对称而产生的。我们测量的光电流始终指向偏振,与薄膜的去偏振无关。测得的光电流的驱动力是由极化电荷在PZT晶界上产生的去极化场[Delimova et al。,Appl。物理来吧91,112907(2007)]。在PbO中间层中受光激发的自由载流子在该场中向产生光电流的电极漂移,这可以作为存在去极化场的标准。结果表明,极化M / PZT / M电容器中的稳态光伏电流(仅测量一年而不重新极化)仅显示30%的下降。这意味着在膜中保留了去极化场的那一年中,产生去极化场的极化电荷没有得到补偿,从而表明极化也得到保留。使用二维现象学模型进行的光电流,去极化场和极化的计算表明,晶界上的极化电荷既不能被自由载流子也不能被带电掺杂剂完全补偿,这证实了实验结果。

著录项

  • 来源
    《Journal of Applied Physics》 |2010年第8期|p.084110.1-084110.7|共7页
  • 作者

    L. A. Delimova; V. S. Yuferev;

  • 作者单位

    Solid State Electronics Division, Ioffe Physicotechnical Institute, Russian Academy of Sciences, 26 Polytekhnicheskaya, St Petersburg, 194021, Russian Federation;

    Solid State Electronics Division, Ioffe Physicotechnical Institute, Russian Academy of Sciences, 26 Polytekhnicheskaya, St Petersburg, 194021, Russian Federation;

  • 收录信息 美国《科学引文索引》(SCI);美国《工程索引》(EI);美国《生物学医学文摘》(MEDLINE);
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  • 正文语种 eng
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