Domain Formation in Ferroelectric Negative Capacitance Devices

M. Hoffmann, S. Slesazeck, T. Mikolajick
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引用次数: 1

Abstract

The use of ferroelectric negative capacitance (NC) has been proposed as a promising way to reduce the power dissipation in nanoscale devices [1]. According to single-domain (SD) Landau theory, a hysteresis-free NC state in a ferroelectric might be stabilized in the presence of depolarization fields below a certain critical film thickness $t_{\mathrm{F, SD}}$. However, it is well-known that depolarization fields will cause the formation of domains in ferroelectrics to reduce the depolarization energy [2], which is rarely considered in the literature on NC [3]. The improvident use of SD Landau theory to model NC devices seems to be the main reason for the large discrepancy between experimental data and the current theory [4]. Here, we will show by simulation how anti-parallel domain formation can strongly limit the stability of the NC state in a metal-ferroelectric-insulator-metal (MFIM) structure, which is schematically shown in Fig. 1.
铁电负电容器件中的畴形成
铁电负电容(NC)被认为是降低纳米级器件功耗的一种很有前途的方法[1]。根据单畴(SD)朗道理论,在退极化场存在下,铁电体中无磁滞的NC态可以稳定在一定的临界薄膜厚度$t_{\ mathm {F, SD}}$下。然而,众所周知,去极化场会导致铁电体中形成畴以降低去极化能[2],这在NC文献中很少被考虑[3]。在对数控装置进行建模时,不谨慎地使用SD朗道理论似乎是造成实验数据与当前理论存在较大差异的主要原因[4]。在这里,我们将通过模拟展示反平行畴的形成如何强烈地限制金属-铁电-绝缘体-金属(MFIM)结构中NC状态的稳定性,如图1所示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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