Zernike Institute for Advanced Materials , Nijenborgh 4, 9747 AG Groningen, The Netherlands.
Stratingh Institute for Chemistry , Nijenborgh 4, 9747 AG Groningen, The Netherlands.
ACS Appl Mater Interfaces. 2017 Aug 16;9(32):27290-27297. doi: 10.1021/acsami.7b06451. Epub 2017 Aug 7.
The parallel-plate capacitor equation is widely used in contemporary material research for nanoscale applications and nanoelectronics. To apply this equation, flat and smooth electrodes are assumed for a capacitor. This essential assumption is often violated for thin-film capacitors because the formation of nanoscale roughness at the electrode interface is very probable for thin films grown via common deposition methods. In this work, we experimentally and theoretically show that the electrical capacitance of thin-film capacitors with realistic interface roughness is significantly larger than the value predicted by the parallel-plate capacitor equation. The degree of the deviation depends on the strength of the roughness, which is described by three roughness parameters for a self-affine fractal surface. By applying an extended parallel-plate capacitor equation that includes the roughness parameters of the electrode, we are able to calculate the excess capacitance of the electrode with weak roughness. Moreover, we introduce the roughness parameter limits for which the simple parallel-plate capacitor equation is sufficiently accurate for capacitors with one rough electrode. Our results imply that the interface roughness beyond the proposed limits cannot be dismissed unless the independence of the capacitance from the interface roughness is experimentally demonstrated. The practical protocols suggested in our work for the reliable use of the parallel-plate capacitor equation can be applied as general guidelines in various fields of interest.
平行板电容器方程在当代纳米应用和纳米电子学的材料研究中被广泛应用。为了应用这个方程,假设电容器的电极是平的和光滑的。然而,对于薄膜电容器来说,这个基本假设经常被违反,因为在通过常见的沉积方法生长的薄膜中,电极界面处形成纳米级粗糙度是非常可能的。在这项工作中,我们通过实验和理论表明,具有实际界面粗糙度的薄膜电容器的电容量比平行板电容器方程预测的值大得多。这种偏差的程度取决于粗糙度的强度,对于自仿射分形表面,可以用三个粗糙度参数来描述。通过应用一个包含电极粗糙度参数的扩展平行板电容器方程,我们能够计算出具有弱粗糙度的电极的额外电容。此外,我们引入了粗糙度参数的限制,在这些限制内,简单的平行板电容器方程对于具有一个粗糙电极的电容器足够准确。我们的结果表明,除非实验证明电容与界面粗糙度无关,否则不能忽略超出建议限制的界面粗糙度。我们工作中提出的用于可靠使用平行板电容器方程的实用协议可以作为各种感兴趣领域的一般指南。