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The impact of rapid thermal annealing for the ferroelectricity of undoped sputtered HfO2 and its wake-up effect

机译:快速热退火对未掺杂溅射HfO2铁电性的影响及其唤醒效应

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摘要

Fundamental aspects of ferroelectric HfO 2, a fluorite-type oxide, are not understood yet. This is evident by different theories regarding, e.g., the wake-up effect or the antiferroelectric-like behavior of HfO 2 manufactured with different doping or deposition techniques. Therefore, we focus on sputtered and undoped HfO 2 to gain deeper understanding of the ferroelectric properties of pure HfO 2. A temperature gradient on a 10×10mm2 substrate during rapid thermal annealing led to different ferroelectric device performances in terms of remnant polarization and the wake-up effect. The results from the electrical characterization are compared to observations by transmission electron microscopy, performed on pristine and trained samples in plan-view as well as in cross section. We observed that different temperature treatments caused effects at the interfaces of the TiN electrodes and also affected the microstructure and defect concentration of the HfO 2 itself. Devices from the hot corner showed wake-up free ferroelectricity with a remnant polarization below 10  μC/cm2, whereas devices from the cold corner showed a strong wake-up effect with remnant polarization starting from 0 to above 20  μC/cm2 after 106 cycles. After observing a small structural transformation in trained devices, we attributed this strong wake-up effect to gradual ferroelastic switching of pristine 110 oriented grains with in-plane polarization to partially out-of-plane polarization, while the predominantly ⟨111⟩ oriented grains in the hot corner can suppress the wake-up effect.
机译:铁电 HfO 2(一种萤石型氧化物)的基本方面尚不清楚。这可以通过不同的理论来证明,例如,用不同的掺杂或沉积技术制造的 HfO 2 的唤醒效应或类反铁电行为。因此,我们专注于溅射和未掺杂的 HfO 2,以更深入地了解纯 HfO 2 的铁电特性。在快速热退火过程中,10×10mm2衬底上的温度梯度导致铁电器件在残余极化和唤醒效应方面的性能不同。将电学表征的结果与透射电子显微镜的观察结果进行比较,透射电子显微镜在平面图和横截面上对原始和经过训练的样品进行观察。我们观察到,不同的温度处理对TiN电极的界面产生了影响,也影响了HfO 2本身的微观结构和缺陷浓度。来自热角的器件表现出无唤醒的铁电性,残余极化低于10 μC/cm2,而来自冷角的器件表现出强烈的唤醒效应,在106次循环后残余极化从0到20 μC/cm2以上。在经过训练的器件中观察到微小的结构转变后,我们将这种强烈的唤醒效应归因于具有面内极化的原始[110]取向晶粒逐渐铁弹性切换为部分面外极化,而热角中主要为⟨111⟩取向的晶粒可以抑制唤醒效应。

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